Kevin Patrick Lannon

Associate Professor Office: (574) 631-7322University of Notre Dame Fax: (574) 631-5952Department of Physics klannon@nd.edu

410 Nieuwland Science HallNotre Dame, Indiana 46556-5670USA

Education

Ph.D. Physics University of Illinois, Urbana-Champaign, 2003

B.A. Physics, Math, and English St. Norbert College, DePere, WI, May 1997.

Experience

Associate Professor, University of Notre Dame, 2014–present.

• Member of the CMS experiment on the LHC at CERN, Geneva, Switzerland

• First observation of the associated production of a Higgs boson with a pair of top quarks.

• First observation of the production of a Z boson in association with a top quark pair.

• Searches for new physics involving top quarks produced in association with W, Z or Hbosons.

• Initiated novel analysis effort to discover new physics using the framework of effectivefield theories (EFT) applied to collisions involving one or more top quarks produced withadditional W, Z, or H bosons.

• Co-Coordinator of University Computing Facilities for the U.S. CMS Collaboration

• Leader of the Online Software Subgroup of the Tracker Data Processing Systems Groupin the CMS Phase 2 Upgrade

• Co-Coordinator of the Software Group for the U.S. CMS Collaboration

• Significant contributions to CMS workflow management software tools

• Continued significant contributions to CMS trigger rate monitoring and operation

• Lead principal investigator for Notre Dame’s Cyberinfrastructure to Accelerate MachineLearning (CAML) GPU cluster

Assistant Professor, University of Notre Dame, 2008–2014.

• Member of the CMS experiment on the LHC at CERN, Geneva, Switzerland

• Computing Liaison to the USCMS Collaboration Board

• Searching for the Higgs boson produced in association with a top quark pair and othernew physics associated with top quarks or Higgs bosons

• Created a Tier 3 computing facility for CMS in collaboration with the ND Center forResearch Computing

• Significant contributions to trigger rate monitoring and trigger development on CMS

Postdoctoral Researcher, The Ohio State University, 2003–2008.

• Member of CDF experiment on the Tevatron Collider at Fermi National Laboratory,Batavia, IL

• CDF Top Quark Properties Working Group Co-Leader, 2006–2007.

• CDF XFT Installation and Commissioning Coordinator, 2005–2006.

• CDF Top Group Code Librarian, 2004–2006.

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• Expert on top quark and Higgs physics, particularly background modeling and estimationtechniques, and multivariate analysis strategies.

• Expert on trigger systems.

Research Assistant, University of Illinois at Urbana-Champaign, 1998–2003.

• Member of the CDF experiment

• Ph.D. Thesis: A Measurement of B Hadron Correlations in pp Collisions at√s = 1.8 TeV.

• Expert in bottom quark production mechanisms

• Expert in muon detector systems

Summer Research Participant, Argonne National Laboratory, Summers 1994–1997.

• Developed unbinned maximum likelihood fitting technique to be used for search foranomalous production for W plus photon events at CDF

• Characterized properties of W and Z plus photon events at CDF

Awards

CAREER Award, National Science Foundation, 2010

Giulio Ascoli Award for Demonstrating Excellence and Originality in the Study of High EnergyPhysics, 2001

Excellence in Teaching Award, University of Illinois, Fall 1997 and Spring 1998

Rev. Patrick N. Butler Award for Excellence in English Studies, 1997

William J. O’Callahan Award in the Arts and Sciences, 1997

Physics Award St. Norbert College, 1997

St. Norbert College Alumni Association Award for Highest Academic Achievement, 1997

GTE Academic All-American Second Team, Cross Country and Track, 1996–1997

English Faculty Endowed Scholarship, St. Norbert College, 1996

Midwest Conference Academic All-Conference, Cross Country, Indoor Track, and OutdoorTrack (12 seasons total), 1994–1997

Distinguished Trustees Scholarship, St. Norbert College, 1993

AffiliationsSigma Pi Sigma, American Physical Society, Division of Particles and Fields, Society of CatholicScientists

Service to the Department

Graduate Recruitment Committee, 2008–2013, 2017–present

High Energy Physics Seminar Organizer, 2008–2013

Computer Committee, 2008–2009, 2010–2011, 2016–present

Undergraduate Curriculum, 2011–2012, 2018–present

Graduate Preliminary Exam Committee, 2012–2014

Graduate Admissions Committee, 2013–present

Graduate Curriculum Committee, 2016–2017

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Service to the College of Science

Computing Committee, 2011–2013

College Council, 2016–present

Organizer for the 2nd Annual Notre Dame Gold Mass, 2018

Honesty Committee, 2018–present

Service to the University

University Committee on First Year Studies, 2013–2016

Center for Research Computing Faculty Advisory Committee, 2016–present

Faculty Affairs, Research, and Scholarship Committee of the Board of Trustees, 2017–present

Service to the Field

Organizing Committee for the U.S. CMS Collaboration Meeting, 2011

Reviewed NSF proposals including CAREER grants, 2011–present

U.S. CMS Collaboration Board Computing Liaison, 2013–2015

Chaired the U.S. CMS Committee to Review Analysis Computing, 2013–2014

U.S. CMS University Computing Facilities Co-Leader, 2015–2019

Co-Chaired the U.S. CMS Tier 2 Budget Reduction Committee, 2015–2016

Organizer for the U.S. CMS Facilities Workshop at the Open Science Grid All-Hands Meet-ing, 2015–2019

Chaired the CMS Workflow Management Review Committee, 2018–2019

CMS Tracker Upgrade Data Processing Systems Software Coordinator, 2018–present

U.S. CMS Software Co-Leader, 2019–present

Organizing Committee for the 2021 Top Quark International Workshop, 2019–present

Faculty Mentoring

Second-Year Faculty Panel, New Faculty Orientation, 2009

NSF CAREER Panel Discussion, Office of Research, 2011

Junior Faculty Mentoring Committee, Prof. Manoel Couder, 2015–2019

Postdoctoral Researchers2009–2013 Jason Slaunwhite Senior Systems Software Engineer at Microfocus Vertica2014–2019 Geoffrey Smith Seeking data science position2015–2019 Kenyi Hurtado HPC Engineer at Notre Dame’s Center for Research Computing

Graduate Students2008–2013 Tessa Pearson∗ Lead ML/AI Engineer in Research at HERE Technologies2008–2014 Wuming Luo Faculty at the Institute of High Energy Physics (IHEP) in Beijing2009–2015 Andrew Brinkerhoff Assistant Professor at Baylor University2011–2017 Charles Mueller Data Scientist at GoGo Inflight Internet2010–2018 Anna Woodard Postdoc in Computer Science at the University of Chicago2014–present Andrew Wightman2016–present Ian McAlister∗∗

2017–present Kelci Mohrman2018–present John Lawrence∗ Co-advised with Prof. Randal Ruchti

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∗∗ Co-advised with Prof. Mitchell Wayne

Undergraduate Students2010 Kathryn Gerbich2010 Shannon Hughes∗

2011–2012 Patrick Marino∗

2010–2013 Kevin McDermott∗

2011–2013 Timothy O’Brien2012–2013 Chris Henneman∗

2013 Hanyi Yi∗

2011–2014 Rachael Creager∗

2012–2014 Anthony Lefeld2012–2014 Christopher Barnes∗

2013–2014 Dillon Bak∗

2014 Bobby Flores∗

2015 Max Kempf∗

2015 Callaghan Commers∗

2015 Eoghan Flannagan∗

2013–2015 William McCormack

2015–2016 John Charters∗

2015–2016 Gregory Greif∗

2015–2016 Colin Dablain2015–2017 Ben Cote∗

2016–2017 Tanner Leighton∗

2016–2017 Ryan Kim∗

2017 Patrick McGuire2014–2018 Kaitlin Salyer∗

2015–2018 Patrick Shields∗

2015–2019 Matthew Drnevich2018–present Kevin Greif∗

2018–present Justin Dragoo∗

2018–present Arianna Garcia∗

2019–present Tianyi Wang∗

2019–present Connor Sabers

∗Co-advised with Prof. Michael Hildreth

REU StudentsIn addition to regularly mentoring students as part of the physics department REU program, I wasco-PI of the Data Intensive Scientific Computing (DISC) REU from 2016-2018 and advised severalstudents through that REU program.

2010 Angela Galvez∗, Kathryn Gerbich (ND)2011 Joshua Hardin∗, Kevin McDermott∗ (ND)2012 Michael Swift∗, Rachael Creager∗ (ND)2013 Edward Varty∗, Hanyi Yi∗ (ND)2014 Samantha Koutsares∗, Patrick Moran∗

2015 Carlos Buxo∗, John Charters∗ (ND), Kaitlin Salyer∗ (ND)2016 Marybeth Beydler, Matthew Link∗∗, Anna Yannakopoulos∗∗, John Charters∗ (ND), Ben

Cote∗ (ND), Colin Dablain∗∗ (ND), Matthew Drnevich∗∗ (ND), Patrick Shields∗ (ND)2017 Ariella Atencio∗, Bryan Harris∗∗, Jessica Stietzel∗∗

2018 Brooke Emison∗, Diego Fernandez∗∗, Khaya Klanot∗∗, Christopher McGrady∗, KevinGreif ∗(ND)

2019 Mary-Ellen Phillips∗, Arianna Garcia∗ (ND), Tianyi Wang∗ (ND)

∗Co-advised with Prof. Michael Hildreth∗∗DISC REU

Grants

• Research in Collider Physics (NSF PHY-0701621)Jan. 2009–May 2011Added as Co-Principal Investigator to ongoing grant, along with four other ND faculty.Total award: $1,920,000

• Research in Collider Physics (NSF PHY-0969524)Aug. 2010–July 2013Co-Principal Investigator along with four other ND faculty.Total award: $2,460,000

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• CAREER: Understanding Particle Masses through Studying Higgs Produced in Associationwith Top Quarks at CMS (NSF PHY-0955765)July 2010–Jun. 2015Sole Principal InvestigatorTotal award: $500,000

• Research in Collider Physics (NSF PHY-1312842)Aug. 2013–July 2016Co-Principal Investigator along with three other ND faculty.Total award: $2,575,000

• CC-NIE Networking Infrastructure: Accelerating Research Data Transit Between the Scien-tist’s Desktop, Campus, and National Cyberinfrastructure (NSF ACI-1340990)Jan. 2014–Dec. 2015Senior personnel; Lead PI is Jaroslaw Nabrzyski along with three other PIs and two othersenior personnel.Total award: $499,935

• REU Site: Data Intensive Scientific Computing (DISC) (NSF IIS-1560363)Feb. 2016–Jan. 2019 Co-Principal Investigator along with one other ND faculty member.Total award: $359,757

• Virtual Clusters for Community Computation (VC3) (DOE DE-SC0015711.0002)Mar. 2016–Feb. 2019Co-Principal Investigator along with three other ND faculty and three non-ND faculty.Total award: $733,481

• Fermi National Laboratory Support for Postdoctoral ResearcherMar. 2015–Mar. 2017Sole Principal InvestigatorTotal award: $89,564

• Research in Collider Physics (NSF PHY-1607578)Sep. 2016–Aug. 2019Co-Principal Investigator along with three other ND faculty.Total award: $2,867,780

• U.S. CMS Operations at the Large Hadron Collider, NSF subaward from PrincetonJan. 2017–Dec. 2022This is a subaward from the NSF cooperative aggreement that funds the U.S. contribution tothe operation. Funds are awarded annually based on negotiated statements of work (SOW).Several ND faculty are co-principal investigators. Here I list the total of the funding receivedto date (through Dec. 31, 2019) for the SOWs in which I’m involved. The total for all NDco-principal investigators is higher.Funding to date: $660,124

• CC* Compute: CAML - Accelerating Machine Learning via Campus and Grid (NSF OAC-1925645)July 2019–Jun. 2021Lead Principal Investigator along with four other ND faculty.Total award: $400,000

• Research in Collider Physics (NSF PHY-1914059)Sep. 2019–Aug. 2022Co-Principal Investigator along with three other ND faculty.Total award: $3,090,000

Invited Talks and Seminars

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Outside Notre Dame

1. “Top Quark Multilepton Signatures as a Window into New Physics,” Michigan State Univer-sity, Oct. 2, 2018

2. “Higgs Physics from the Bottom Down (Higgs physics beyond ttH),” 11th International Work-shop on Top Quark Physics (TOP 2018), Bad Neuenahr, Germany, Sep. 20, 2018

3. “Recent Top Physics Results from CMS,” Lake Louise Winter Institute, Canada, Feb. 19,2018

4. “Big Data Leads to Big Discoveries at the LHC,” Colloquium for the Physics and ComputerScience Departments at College of the Holy Cross, Worcester, MA, Nov. 2, 2017

5. “Associated Production of Bosons and Top Quark Pairs as a Window on New Physics,” CornellUniversity, Oct. 28, 2016

6. “VC3 - R&D for Virtual Clusters,” Open Science Grid All Hands Meeting, Clemson University,Mar. 15, 2016

7. “Top Quark Physics,” Meeting of the Division of Particles and Fields of the American PhysicalSociety, Ann Arbor, MI, Aug. 5, 2015

8. “Search for Higgs Produced in Association with Top Quark Pairs,” Argonne National Labo-ratory, Nov. 26, 2013

9. “Search for Higgs Produced in Association with Top Quark Pairs,” Karlsruhe Institute ofTechnology, Karlsruhe, Germany, Oct. 24, 2013

10. “Search for Higgs Produced in Association with Top Quark Pairs,” Deutsches Elektronen-Synchrotron (DESY) Laboratory, Hamburg, Germany, Oct. 23, 2013

11. “Search for Higgs Produced in Association with Top Quark Pairs,” University of Illinois atUrbana-Champaign, Oct. 7, 2013

12. “Backgrounds to Top Pair Associated Higgs Production and MC Tools,” 6th InternationalWorkshop on Top Quark Physics, Durbach, Germany, Sep. 18, 2013

13. “Recent Results from CMS,” SLAC Summer Institute, Jul. 9, 2013

14. “Higgs Decaying into Bottom Quarks,” Higgs Coupling Conference, Tokyo, Japan, Nov. 18,2012

15. “Search for Higgs Produced in Association with Top Quark Pairs,” Purdue University, Nov.6, 2012

16. “Search for Higgs Produced in Association with Top Quark Pairs,” University of Wisconsin,Oct. 30, 2012

17. “ttH at CMS and ATLAS,” CERN Collider Cross Talk series, Geneva, Switzerland, Oct. 18,2012

18. “Search for Higgs Produced in Association with Top Quark Pairs,” Indiana University, Oct.22, 2012

19. “Search for Higgs Produced in Association with Top Quark Pairs,” Michigan State University,Sep. 25, 2012

20. “Search for Higgs Produced in Association with Top Quark Pairs,” University of Michigan,Sep. 24, 2012

21. “CMS Status,” 4th International Workshop on Top Quark Physics, Sant Feliu de Guixols,Spain, Sep. 26, 2011

22. “Top Physics with CMS,” Conference on First LHC Data, University of Michigan, Dec. 13,2010

23. “Observation of Single Top at CDF,” CERN Joint EP/PP Seminar, Geneva, Switzerland, Mar.31, 2009

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24. “Measurement of Single Top Quark Production at CDF,” University of Wisconsin-Madison,Apr. 14, 2008

25. “Digging Up Top and Higgs at CDF,” Colloquium, University of Nebraska-Lincoln, Mar. 31,2008

26. “Digging Up Top and Higgs at CDF,” Colloquium, Iowa State University, Mar. 10, 2008

27. “Pushing the Limits: From Top to Higgs at CDF,” University of California-Davis, Feb. 26,2008

28. “Pushing the Limits: From Top to Higgs at CDF,” University of Massachusetts-Amherst, Feb.22, 2008

29. “Pushing the Limits: From Top to Higgs at CDF,” Fermi National Accelerator Laboratory,Feb. 15, 2008

30. “Digging Up Top and Higgs at CDF,” Colloquium, University of Illinois-Chicago, Feb. 13,2008

31. “Top Quark Physics at the Tevatron,” Fermilab Users’ Meeting, Jun. 6, 2007

32. “Recent Measurements of the Top Quark from Fermilab,” April APS Meeting, Apr. 15, 2007

33. “Search for New Phenomena in the CDF Top Quark Sample,” Southern Methodist University,Feb. 5, 2007

34. “Search for New Phenomena in the CDF Top Quark Sample,” University of Illinois at Urbana-Champaign HETEP, Jan. 29, 2007

35. “Search for New Phenomena in the CDF Top Quark Sample,” Argonne National LaboratoryHEP Division, Oct. 11, 2006

36. “Search for New Phenomena in the CDF Top Quark Sample,” SUSY 06, 14th InternationalConference on Supersymmetry, and the Unification of Fundamental Interactions, Jun. 12, 2006

37. “Search for Single-Top Production at CDF,” PHENO 06 Symposium, May 16, 2006

38. “Measuring B Hadron Correlations at CDF,” The Ohio State University, Jun. 18, 2003

Within Notre Dame Community, Including Public Lectures

1. “Big Data Leads to Big Discoveries at the LHC,” Quarknet Summer Lunchtime Talks, July16, 2019

2. “Big Data Leads to Big Discoveries at the LHC,” CRC Summer Scholars program, July 2,2019

3. “Discovering the Other 95% of the Universe: What’s Next at the LHC?” Junior Parents’Weekend, February 16, 2019

4. “Big Data Leads to Big Discoveries at the LHC,” Quarknet Summer Lunchtime Talks, July 6,2018

5. “Big Data Leads to Big Discoveries at the LHC,” CRC Summer Scholars program, July 2,2018

6. “Deep Learning,” Machine Learning Workshop, Center for Research Computing, June 22,2018.

7. “The Martian,” Warrior Scholars Program, June 15, 2018.

8. “Big Data Leads to Big Discoveries at the LHC,” DISC REU Lunch Seminar, May 31, 2018

9. “Discovering the Other 95% of the Universe: What’s Next at the LHC,” Junior Parents’Weekend, February 17, 2018

10. “Deep Learning,” DISC REU Training Seminar, July 19, 2017.

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11. “Big Data Leads to Big Discoveries at the LHC,” CRC Summer Scholars program, June 302017

12. “Big Data Leads to Big Discoveries at the LHC,” DISC REU Lunch Seminar, June 8, 2017

13. “Discovering the Other 95% of the Universe: What’s Next at the LHC,” Junior Parents’Weekend, February 18, 2017

14. “Big Data Leads to Big Discoveries at the LHC,” CRC Summer Scholars program, July 5,2016

15. “Deep Learning,” DISC REU Training Seminar, June 15, 2016.

16. “Big Data Leads to Big Discoveries at the LHC,” DISC REU Lunch Seminar, May 26, 2016

17. “CMS Data Analysis with Lobster and Workqueue,” Cooperative Computing LaboratoryWorkshop, Oct. 19, 2016

18. “Discovering the Other 95% of the Universe: What’s Next for the LHC,” Our Universe Re-vealed Public Lecture Series, Oct. 6, 2016

19. “Discovering the Other 95% of the Universe: What’s Next at the LHC,” Junior Parents’Weekend, February 20, 2016

20. “After the Higgs: Discovering the Other 95% of the Universe,” Notre Dame Physics REUSeminar, July 8, 2015

21. “Discovering the Other 95% of the Universe: True Stories From the Energy Frontier,” JuniorParents’ Weekend, February 21, 2015

22. “Big Data Leads to Big Discovery: A New Particle Discovered at the LHC,” CRC SummerScholars program, July 7, 2014

23. “After the Higgs: Discovering the Other 95% of the Universe,” Notre Dame Physics REUSeminar, May 28, 2014

24. “Searching for the Other 95% of the Universe: True Stories From the Energy Frontier”, TEDx-UND, Feb. 27, 2014

25. “Big Data Leads to Big Discovery: A New Particle Discovered at the LHC,” CRC SummerScholars program, July 8, 2013

26. “Scaling Up CMS Tier-3 Data Processing,” Cooperative Computing Laboratory Workshop,Oct. 11, 2012

27. “The Higgs Boson: Beyond the Headlines,” Nieuwland Lecture Series, Sep. 6, 2012

28. “Notre Dame Science and the Higgs Boson,” Notre Dame Leadership Seminar, Jul. 26, 2012

29. “The Big Higgs Announcement: What Does it Mean?”, Notre Dame Physics REU Seminar,Jul. 19, 2012

30. “How Grid Computing Helped to Discover the Higgs Boson,” Notre Dame Center for ResearchComputing Summer Scholars Program, Jul. 16, 2012

31. “LHC: Searching for the Other 96% of the Universe,” Scientia Presentation, Sep. 15, 2011

32. “Particle Physics on the Grid: The CERN CMS Experiment at Notre Dame,” Notre DameCenter for Research Computing Summer Scholars Program, Jun. 20, 2011

33. “What’s the Big Deal About the Higgs,” Notre Dame Physics REU Seminar, Jul. 28, 2010

34. “Last Lecture,” Last Lecture Series, Dec. 2, 2010

PublicationsIn the field of particle physics, it is customary to list all members of an experimental collaboration inalphabetical order (in some cases first sorted by institution). Below is a list of selected publicationsin which I played a significant role, either as a primary author or as an important contributor. Afterthis, I give my full list of publications.

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Selected Publications

Refereed Journals

1. A. M. Sirunyan et al. [CMS Collaboration], “Observation of ttH production,” Phys. Rev. Lett.120, no. 23, 231801 (2018) [17 pages] [Impact Factor: 9.227]doi:10.1103/PhysRevLett.120.231801,10.1130/PhysRevLett.120.231801 [arXiv:1804.02610 [hep-ex]]

2. A. M. Sirunyan et al. [CMS Collaboration], “Evidence for associated production of a Higgsboson with a top quark pair in final states with electrons, muons, and hadronically decayingτ leptons at

√s = 13 TeV,” JHEP 1808, 066 (2018) [50 pages] [Impact Factor: 5.833]

doi:10.1007/JHEP08(2018)066 [arXiv:1803.05485 [hep-ex]]

3. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of the cross section for top quarkpair production in association with a W or Z boson in proton-proton collisions at

√s = 13

TeV,” JHEP 1808, 011 (2018) [46 pages] [Impact Factor: 5.833]doi:10.1007/JHEP08(2018)011 [arXiv:1711.02547 [hep-ex]]

4. V. Khachatryan et al. [CMS Collaboration], “Observation of top quark pairs produced inassociation with a vector boson in pp collisions at

√s = 8 TeV,” JHEP 1601, 096 (2016) [52

pages] [Impact Factor: 5.833]doi:10.1007/JHEP01(2016)096 [arXiv:1510.01131 [hep-ex]]

5. V. Khachatryan et al. [CMS Collaboration], “Search for the associated production of the Higgsboson with a top-quark pair,” JHEP 1409, 087 (2014) [Erratum-ibid. 1410, 106 (2014)] [64pages] [Impact Factor: 5.833][arXiv:1408.1682 [hep-ex]]

6. S. Chatrchyan et al. [CMS Collaboration], “Search for a standard-model-like Higgs boson witha mass in the range 145 to 1000 GeV at the LHC,” Eur. Phys. J. C 73, 2469 (2013) [43 pages][Impact Factor: 4.843][arXiv:1304.0213 [hep-ex]]

7. S. Chatrchyan et al. [CMS Collaboration], “Observation of a new boson with mass near 125GeV in pp collisions at

√s = 7 and 8 TeV,” JHEP 1306, 081 (2013) [117 pages] [Impact

Factor: 5.833] [arXiv:1303.4571 [hep-ex]]. [Impact Factor: 5.618]

8. S. Chatrchyan et al. [CMS Collaboration], “Search for the standard model Higgs boson pro-duced in association with a top-quark pair in pp collisions at the LHC,” JHEP 1305, 145(2013) [44 pages] [Impact Factor: 5.833][arXiv:1303.0763 [hep-ex]]

9. K. Lannon, F. Margaroli and C. Neu, “Measurements of the Production, Decay and Propertiesof the Top Quark: A Review,” Eur. Phys. J. C 72, 2120 (2012) [22 pages] [Impact Factor:4.843][arXiv:1201.5873 [hep-ex]]

10. S. Chatrchyan et al. [CMS Collaboration], “A New Boson with a Mass of 125 GeV Observedwith the CMS Experiment at the Large Hadron Collider,” Science 338, 1569 (2012). [7 pages][Impact Factor: 41.04]doi:10.1126/science.1230816

11. S. Chatrchyan et al. [CMS Collaboration], “Observation of a new boson at a mass of 125GeV with the CMS experiment at the LHC,” Phys. Lett. B 716, 30 (2012) [32 pages] [ImpactFactor: 4.162][arXiv:1207.7235 [hep-ex]]

12. T. Aaltonen et al. [CDF Collaboration], “Search for Standard Model Higgs Boson Productionin Association with a W Boson at CDF,” Phys. Rev. D 85, 052002 (2012) [49 pages] [Impact

9

Factor: 4.368][arXiv:1112.1930 [hep-ex]]

13. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the tt Production Cross Sectionin pp Collisions at

√s = 7 TeV using the Kinematic Properties of Events with Leptons and

Jets,” Eur. Phys. J. C 71, 1721 (2011) [39 pages] [Impact Factor: 4.843][arXiv:1106.0902 [hep-ex]]

14. T. Aaltonen et al. [CDF Collaboration], “Observation of Single Top Quark Production andMeasurement of |Vtb| with CDF,” Phys. Rev. D82, 112005 (2010). [62 pages] [Impact Factor:4.368][arXiv:1004.1181 [hep-ex]]

15. T. Aaltonen et al. [CDF Collaboration], “First Measurement of the Ratio σtt/σZ/γ∗→`` andPrecise Extraction of the tt Cross Section,” Phys. Rev. Lett. 105, 012001 (2010). [7 pages][Impact Factor: 9.227][arXiv:1004.3224 [hep-ex]]

16. T. Aaltonen et al. [CDF Collaboration], “Search for a Higgs Boson produced in association aW Boson in ppCollisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 103, 101802 (2009). [7 pages]

[Impact Factor: 9.227][arXiv:0906.5613 [hep-ex]]

17. T. Aaltonen et al. [CDF Collaboration], “Observation of Electroweak Single Top Quark Pro-duction,” Phys. Rev. Lett. 103, 092002 (2009). [9 pages] [Impact Factor: 9.227][arXiv:0903.0885 [hep-ex]]

18. T. Aaltonen et al. [CDF Collaboration], “Search for Standard Model Higgs Boson Productionin Association with a W Boson using a Neural Network Discriminant at CDF,” Phys. Rev.D80, 012002 (2009). [17 pages] [Impact Factor: 4.368][arXiv:0905.3155 [hep-ex]]

19. T. Aaltonen et al. [CDF Collaboration], “Search for the Production of Narrow t anti-b Res-onances in 1.9 fb−1 of ppCollisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 103, 041801 (2009).

[7 pages] [Impact Factor: 9.227][arXiv:0902.3276 [hep-ex]]

20. T. Aaltonen et al. [CDF Collaboration], “Search for Heavy Top-like Quarks Using LeptonPlus Jets Events in 1.96-TeV pp Collisions,” Phys. Rev. Lett. 100, 161803 (2008). [7 pages][Impact Factor: 9.227][arXiv:0801.3877 [hep-ex]]

21. D. E. Acosta et al. [CDF Collaboration], “Measurement of the cross section for tt productionin pp collisions using the kinematics of lepton + jets events,” Phys. Rev. D72, 052003 (2005).[45 pages] [Impact Factor: 4.368][hep-ex/0504053]

22. D. E. Acosta et al. [CDF Collaboration], “Measurements of bb azimuthal production correla-tions in pp collisions at

√s = 1.8 TeV,” Phys. Rev. D71, 092001 (2005). [38 pages] [Impact

Factor: 4.368][hep-ex/0412006]

Conference Proceedings

23. J. Stietzel and K. Lannon, “Study of Neural Network Size Requirements for ApproximatingFunctions Relevant to HEP,” to be published in the proceedings of the 23rd InternationalConference on Computing in High Energy and Nuclear Physics. [8 pages]

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24. K. Albertsson et al., “Machine Learning in High Energy Physics Community White Pa-per,” J. Phys. Conf. Ser. 1085, no. 2, 022008 (2018) doi:10.1088/1742-6596/1085/2/022008[arXiv:1807.02876 [physics.comp-ph]]. [27 pages]

25. P. Ivie, C. Zheng, K. Lannon and D. Thain, “An analysis of reproducibility and non-determinismin HEP software and ROOT data,” J. Phys. Conf. Ser. 898, no. 10, 102007 (2017). doi:10.1088/1742-6596/898/10/102007 [8 pages]

26. M. Wolf et al., “Scaling up a CMS tier-3 site with campus resources and a 100 Gb/s net-work connection: what could go wrong?,” J. Phys. Conf. Ser. 898, no. 8, 082041 (2017).doi:10.1088/1742-6596/898/8/082041 [8 pages]

27. M. Wolf et al., “Opportunistic Computing with Lobster: Lessons Learned from Scaling up to25k Non-Dedicated Cores,” J. Phys. Conf. Ser. 898, no. 5, 052036 (2017). doi:10.1088/1742-6596/898/5/052036 [8 pages]

28. J. Balcas et al., “CMS Connect,” J. Phys. Conf. Ser. 898, no. 8, 082032 (2017). doi:10.1088/1742-6596/898/8/082032 [7 pages]

29. E. Bartz et al., “FPGA-Based Tracklet Approach to Level-1 Track Finding at CMS for the HL-LHC,” EPJ Web Conf. 150, 00016 (2017) doi:10.1051/epjconf/201715000016 [arXiv:1706.09225[physics.ins-det]]. [11 pages]

30. E. Bartz et al., “FPGA-Based Real-Time Charged Particle Trajectory Reconstruction at theLarge Hadron Collider,” doi:10.1109/FCCM.2017.27 [8 pages]

31. A. Woodard et al., “Exploiting volatile opportunistic computing resources with Lobster,” J.Phys. Conf. Ser. 664, no. 3, 032035 (2015). doi:10.1088/1742-6596/664/3/032035 [7 pages]

32. A. Woodard et al., “Scaling Data Intensive Physics Applications to 10k Cores on Non-dedicatedClusters with Lobster,” doi:10.1109/CLUSTER.2015.53 [10 pages]

33. T. Aaltonen et al. [CDF and D0 Collaborations], “Combined CDF and D0 Upper Limitson Standard Model Higgs Boson Production with up to 8.2 fb−1 of Data,” [arXiv:1103.3233[hep-ex]]. [34 pages]

34. A. Abulencia et al. [CDF Collaboration], “eXtremely Fast Tracker Trigger Upgrade at CDF,”Nucl. Instrum. Meth. A 598, 328 (2009). doi:10.1016/j.nima.2008.08.034 [3 pages]

35. R. C. Group et al. [CDF Collaboration], “Combination of Single Top Quark ProductionResults from CDF,” [arXiv:0809.4670 [hep-ex]]. [3 pages]

36. I. Fedorko et al. [CDF Collaboration], “The CDF II eXtremely Fast Tracker Upgrade,”doi:10.1142/9789812819093 0159 [6 pages]

37. A. Abulencia et al., “The CDF II 3D-Track Level 2 Trigger Upgrade,” doi:10.1109/RTC.2007.4382819[8 pages]

38. A. Abulencia et al., “The CDF II eXtremely Fast Tracker Upgrade,” Nucl. Instrum. Meth. A581, no. 1-2, 482 (2007). doi:10.1016/j.nima.2007.08.032 [3 pages]

39. K. Lannon [CDF Collaboration], “Search for new phenomena in the CDF top quark sample,”AIP Conf. Proc. 903, no. 1, 109 (2007) doi:10.1063/1.2735137 [hep-ex/0612009]. [4 pages]

Full Publication List (refereed journals only)

Below is the full list of publications on which I am an author by virtue of my membership in eitherthe CMS or CDF collaborations. The publications are grouped by collaboration.

Also included is a table summarizing the impact factors of all journals in the list below, includingthe number of publications from the list appearing in each journal. The table is sorted by the impactfactor of the journals.

11

Journal Impact Factor Number of PublicationsNature 43.070 1Science 41.04 1

Nature Physics 20.113 1Physical Review Letters 9.227 330

Journal Of High Energy Physics 5.833 299European Physical Journal C 4.843 119

Physical Review D 4.368 319Physics Letters B 4.162 216

Journal Of Physics G 3.534 1Physical Review C 3.132 12Annals of Physics 2.267 2

Nuclear Instruments and Methods A 1.433 2Journal of Instrumentation 1.366 46Modern Physics Letters A 1.367 1

IEEE Transactions On Nuclear Science 1.219 1

CMS

40. A. M. Sirunyan et al. [CMS Collaboration], “Search for a low-mass τ+τ− resonance in asso-ciation with a bottom quark in proton-proton collisions at

√s = 13 TeV,” JHEP 1905, 210

(2019) [39 pages]doi:10.1007/JHEP05(2019)210 [arXiv:1903.10228 [hep-ex]]

41. A. M. Sirunyan et al. [CMS Collaboration], “Search for supersymmetry in final states withphotons and missing transverse momentum in proton-proton collisions at 13 TeV,” JHEP1906, 143 (2019) [5 pages][arXiv:1903.07070 [hep-ex]]

42. A. M. Sirunyan et al. [CMS Collaboration], “Performance of missing transverse momentumreconstruction in proton-proton collisions at

√s = 13 TeV using the CMS detector,” JINST

14, no. 07, P07004 (2019) [55 pages]doi:10.1088/1748-0221/14/07/P07004 [arXiv:1903.06078 [hep-ex]]

43. A. M. Sirunyan et al. [CMS Collaboration], “An embedding technique to determine ττ back-grounds in proton-proton collision data,” JINST 14, no. 06, P06032 (2019) [57 pages]doi:10.1088/1748-0221/14/06/P06032 [arXiv:1903.01216 [hep-ex]]

44. A. M. Sirunyan et al. [CMS Collaboration], “Search for a heavy pseudoscalar boson decayingto a Z and a Higgs boson at

√s = 13 TeV,” Eur. Phys. J. C 79, 564 (2019) [39 pages]

doi:10.1140/epjc/s10052-019-7058-z [arXiv:1903.00941 [hep-ex]]

45. M. Aaboud et al. [ATLAS and CMS Collaborations], “Combinations of single-top-quark pro-duction cross-section measurements and |fLVVtb| determinations at

√s = 7 and 8 TeV with

the ATLAS and CMS experimentsCombinations of single-top-quark production cross-sectionmeasurements and —fLV Vtb— determinations at

√s = 7 and 8 TeV with the ATLAS and

CMS experiments,” JHEP 1905, 088 (2019) [81 pages]doi:10.1007/JHEP05(2019)088 [arXiv:1902.07158 [hep-ex]]

46. A. M. Sirunyan et al. [CMS Collaboration], “Observation of Two Excited B+c States and

Measurement of the B+c (2S) Mass in pp Collisions at

√s = 13 TeV,” Phys. Rev. Lett. 122,

no. 13, 132001 (2019) [17 pages]doi:10.1103/PhysRevLett.122.132001 [arXiv:1902.00571 [hep-ex]]

47. A. M. Sirunyan et al. [CMS Collaboration], “Search for W boson decays to three chargedpions,” Phys. Rev. Lett. 122, no. 15, 151802 (2019) [17 pages]doi:10.1103/PhysRevLett.122.151802 [arXiv:1901.11201 [hep-ex]]

12

48. A. M. Sirunyan et al. [CMS Collaboration], “Search for supersymmetry in events with a pho-ton, jets, b -jets, and missing transverse momentum in protonproton collisions at 13 TeV,”Eur. Phys. J. C 79, no. 5, 444 (2019) [39 pages]doi:10.1140/epjc/s10052-019-6926-x,10.1016/epjc/s10052-019-6926-x [arXiv:1901.06726 [hep-ex]]

49. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of electroweak WZ boson produc-tion and search for new physics in WZ + two jets events in pp collisions at

√s = 13TeV,”

Phys. Lett. B 795, 281 (2019) [27 pages]doi:10.1016/j.physletb.2019.05.042 [arXiv:1901.04060 [hep-ex]]

50. A. M. Sirunyan et al. [CMS Collaboration], “Measurements of the pp → WZ inclusive anddifferential production cross section and constraints on charged anomalous triple gauge cou-plings at

√s = 13 TeV,” JHEP 1904, 122 (2019) [61 pages]

doi:10.1007/JHEP04(2019)122 [arXiv:1901.03428 [hep-ex]]

51. A. M. Sirunyan et al. [CMS Collaboration], “Measurements of the Higgs boson width andanomalousHV V couplings from on-shell and off-shell production in the four-lepton final state,”Phys. Rev. D 99, no. 11, 112003 (2019) [33 pages]doi:10.1103/PhysRevD.99.112003 [arXiv:1901.00174 [hep-ex]]

52. A. M. Sirunyan et al. [CMS Collaboration], “Search for dark matter produced in associationwith a single top quark or a top quark pair in proton-proton collisions at

√s = 13 TeV,” JHEP

1903, 141 (2019) [43 pages]doi:10.1007/JHEP03(2019)141 [arXiv:1901.01553 [hep-ex]]

53. A. M. Sirunyan et al. [CMS Collaboration], “Search for the pair production of light top squarksin the e±µ∓ final state in proton-proton collisions at

√s = 13 TeV,” JHEP 1903, 101 (2019)

[39 pages]doi:10.1007/JHEP03(2019)101 [arXiv:1901.01288 [hep-ex]]

54. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of the top quark mass in the all-jetsfinal state at

√s = 13 TeV and combination with the lepton+jets channel,” Eur. Phys. J. C

79, no. 4, 313 (2019) [39 pages]doi:10.1140/epjc/s10052-019-6788-2 [arXiv:1812.10534 [hep-ex]]

55. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of the tt production cross section,the top quark mass, and the strong coupling constant using dilepton events in pp collisions at√s = 13 TeV,” Eur. Phys. J. C 79, no. 5, 368 (2019) [53 pages]

doi:10.1140/epjc/s10052-019-6863-8 [arXiv:1812.10505 [hep-ex]]

56. A. M. Sirunyan et al. [CMS Collaboration], “Search for vector-like quarks in events with twooppositely charged leptons and jets in proton-proton collisions at

√s = 13 TeV,” Eur. Phys.

J. C 79, no. 4, 364 (2019) [43 pages]doi:10.1140/epjc/s10052-019-6855-8 [arXiv:1812.09768 [hep-ex]]

57. A. M. Sirunyan et al. [CMS Collaboration], “Search for contact interactions and large extradimensions in the dilepton mass spectra from proton-proton collisions at

√s = 13 TeV,” JHEP

1904, 114 (2019) [35 pages]doi:10.1007/JHEP04(2019)114 [arXiv:1812.10443 [hep-ex]]

58. A. M. Sirunyan et al. [CMS Collaboration], “Search for a heavy resonance decaying to a topquark and a vector-like top quark in the lepton+jets final state in pp collisions at

√s = 13

TeV,” Eur. Phys. J. C 79, no. 3, 208 (2019) [45 pages]doi:10.1140/epjc/s10052-019-6688-5 [arXiv:1812.06489 [hep-ex]]

59. A. M. Sirunyan et al. [CMS Collaboration], “Measurement and interpretation of differentialcross sections for Higgs boson production at

√s = 13 TeV,” Phys. Lett. B 792, 369 (2019) [28

pages]doi:10.1016/j.physletb.2019.03.059 [arXiv:1812.06504 [hep-ex]]

13

60. A. M. Sirunyan et al. [CMS Collaboration], “Inclusive search for supersymmetry in pp collisionsat√s = 13 TeV using razor variables and boosted object identification in zero and one lepton

final states,” JHEP 1903, 031 (2019) [63 pages]doi:10.1007/JHEP03(2019)031 [arXiv:1812.06302 [hep-ex]]

61. A. M. Sirunyan et al. [CMS Collaboration], “Search for an exotic decay of the Higgs boson toa pair of light pseudoscalars in the final state with two muons and two b quarks in pp collisionsat 13 TeV,” Phys. Lett. B 795, 398 (2019) [26 pages]doi:10.1016/j.physletb.2019.06.021 [arXiv:1812.06359 [hep-ex]]

62. A. M. Sirunyan et al. [CMS Collaboration], “Observation of Single Top Quark Production inAssociation with a Z Boson in Proton-Proton Collisions at

√s =13 TeV,” Phys. Rev. Lett.

122, no. 13, 132003 (2019) [19 pages]doi:10.1103/PhysRevLett.122.132003 [arXiv:1812.05900 [hep-ex]]

63. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of the energy density as a functionof pseudorapidity in proton-proton collisions at

√s = 13 TeV,” Eur. Phys. J. C 79, no. 5, 391

(2019) [35 pages]doi:10.1140/epjc/s10052-019-6861-x [arXiv:1812.04095 [hep-ex]]

64. A. M. Sirunyan et al. [CMS Collaboration], “Search for supersymmetry in events with aphoton, a lepton, and missing transverse momentum in proton-proton collisions at

√s = 13

TeV,” JHEP 1901, 154 (2019) [37 pages]doi:10.1007/JHEP01(2019)154 [arXiv:1812.04066 [hep-ex]]

65. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of inclusive very forward jet crosssections in proton-lead collisions at

√sNN = 5.02 TeV,” JHEP 1905, 043 (2019) [36 pages]

doi:10.1007/JHEP05(2019)043 [arXiv:1812.01691 [hep-ex]]

66. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of associated production of a Wboson and a charm quark in proton-proton collisions at

√s = 13 TeV,” Eur. Phys. J. C 79,

no. 3, 269 (2019) [43 pages]doi:10.1140/epjc/s10052-019-6752-1 [arXiv:1811.10021 [hep-ex]]

67. A. M. Sirunyan et al. [CMS Collaboration], “Search for dark matter in events with a leptoquarkand missing transverse momentum in proton-proton collisions at 13 TeV,” Phys. Lett. B 795,76 (2019) [24 pages]doi:10.1016/j.physletb.2019.05.046 [arXiv:1811.10151 [hep-ex]]

68. A. M. Sirunyan et al. [CMS Collaboration], “Search for resonant production of second-generation sleptons with same-sign dimuon events in proton-proton collisions at

√s = 13

TeV,” Eur. Phys. J. C 79, no. 4, 305 (2019) [39 pages]doi:10.1140/epjc/s10052-019-6800-x [arXiv:1811.09760 [hep-ex]]

69. A. M. Sirunyan et al. [CMS Collaboration], “Search for associated production of a Higgs bosonand a single top quark in proton-proton collisions at

√s = TeV,” Phys. Rev. D 99, no. 9,

092005 (2019) [29 pages]doi:10.1103/PhysRevD.99.092005 [arXiv:1811.09696 [hep-ex]]

70. A. M. Sirunyan et al. [CMS Collaboration], “Combination of searches for Higgs boson pairproduction in proton-proton collisions at

√s = 13 TeV,” Phys. Rev. Lett. 122, no. 12, 121803

(2019) [18 pages]doi:10.1103/PhysRevLett.122.121803 [arXiv:1811.09689 [hep-ex]]

71. A. M. Sirunyan et al. [CMS Collaboration], “Search for a standard model-like Higgs boson inthe mass range between 70 and 110 GeV in the diphoton final state in proton-proton collisionsat√s = 8 and 13 TeV,” Phys. Lett. B 793, 320 (2019) [28 pages]

doi:10.1016/j.physletb.2019.03.064 [arXiv:1811.08459 [hep-ex]]

72. A. M. Sirunyan et al. [CMS Collaboration], “Search for long-lived particles decaying intodisplaced jets in proton-proton collisions at

√s = 13 TeV,” Phys. Rev. D 99, no. 3, 032011

14

(2019) [28 pages]doi:10.1103/PhysRevD.99.032011 [arXiv:1811.07991 [hep-ex]]

73. A. M. Sirunyan et al. [CMS Collaboration], “Search for a W? boson decaying to a vector-likequark and a top or bottom quark in the all-jets final state,” JHEP 1903, 127 (2019) [39 pages]doi:10.1007/JHEP03(2019)127 [arXiv:1811.07010 [hep-ex]]

74. A. M. Sirunyan et al. [CMS Collaboration], “Measurements of tt differential cross sections inproton-proton collisions at

√s = 13 TeV using events containing two leptons,” JHEP 1902,

149 (2019) [103 pages]doi:10.1007/JHEP02(2019)149 [arXiv:1811.06625 [hep-ex]]

75. A. M. Sirunyan et al. [CMS Collaboration], “Search for dark matter produced in associationwith a Higgs boson decaying to a pair of bottom quarks in protonproton collisions at

√s =

13 TeV,” Eur. Phys. J. C 79, no. 3, 280 (2019) [43 pages]doi:10.1140/epjc/s10052-019-6730-7 [arXiv:1811.06562 [hep-ex]]

76. A. M. Sirunyan et al. [CMS Collaboration], “Search for excited leptons in ``γ final states inproton-proton collisions at

√s = 13 TeV,” JHEP 1904, 015 (2019) [35 pages]

doi:10.1007/JHEP04(2019)015 [arXiv:1811.03052 [hep-ex]]

77. A. M. Sirunyan et al. [CMS Collaboration], “Search for pair production of first-generationscalar leptoquarks at

√s = 13 TeV,” Phys. Rev. D 99, no. 5, 052002 (2019) [28 pages]

doi:10.1103/PhysRevD.99.052002 [arXiv:1811.01197 [hep-ex]]

78. A. M. Sirunyan et al. [CMS Collaboration], “Search for heavy neutrinos and third-generationleptoquarks in hadronic states of two τ leptons and two jets in proton-proton collisions at√s = 13 TeV,” JHEP 1903, 170 (2019) [39 pages]

doi:10.1007/JHEP03(2019)170 [arXiv:1811.00806 [hep-ex]]

79. A. M. Sirunyan et al. [CMS Collaboration], “Search for nonresonant Higgs boson pair produc-tion in the bbbb final state at

√s = 13 TeV,” JHEP 1904, 112 (2019) [45 pages]

doi:10.1007/JHEP04(2019)112 [arXiv:1810.11854 [hep-ex]]

80. A. M. Sirunyan et al. [CMS Collaboration], “Search for low-mass resonances decaying intobottom quark-antiquark pairs in proton-proton collisions at

√s = 13 TeV,” Phys. Rev. D 99,

no. 1, 012005 (2019) [25 pages]doi:10.1103/PhysRevD.99.012005 [arXiv:1810.11822 [hep-ex]]

81. A. M. Sirunyan et al. [CMS Collaboration], “Search for rare decays of Z and Higgs bosons toJ/ψ and a photon in proton-proton collisions at

√s = 13 TeV,” Eur. Phys. J. C 79, no. 2, 94

(2019) [37 pages]doi:10.1140/epjc/s10052-019-6562-5 [arXiv:1810.10056 [hep-ex]]

82. A. M. Sirunyan et al. [CMS Collaboration], “Search for new particles decaying to a jet and anemerging jet,” JHEP 1902, 179 (2019) [39 pages]doi:10.1007/JHEP02(2019)179 [arXiv:1810.10069 [hep-ex]]

83. A. M. Sirunyan et al. [CMS Collaboration], “Search for pair-produced three-jet resonances inproton-proton collisions at

√s =13 TeV,” Phys. Rev. D 99, no. 1, 012010 (2019) [33 pages]

doi:10.1103/PhysRevD.99.012010 [arXiv:1810.10092 [hep-ex]]

84. A. M. Sirunyan et al. [CMS Collaboration], “Search for resonant tt production in proton-proton collisions at

√s = 13 TeV,” JHEP 1904, 031 (2019) [53 pages]

doi:10.1007/JHEP04(2019)031 [arXiv:1810.05905 [hep-ex]]

85. A. M. Sirunyan et al. [CMS Collaboration], “Search for top quark partners with charge 5/3in the same-sign dilepton and single-lepton final states in proton-proton collisions at

√s = 13

TeV,” JHEP 1903, 082 (2019) [43 pages]doi:10.1007/JHEP03(2019)082 [arXiv:1810.03188 [hep-ex]]

15

86. A. M. Sirunyan et al. [CMS Collaboration], “Observation of prompt J/ψ meson elliptic flowin high-multiplicity pPb collisions at

√sNN = 8.16 TeV,” Phys. Lett. B 791, 172 (2019) [23

pages]doi:10.1016/j.physletb.2019.02.018 [arXiv:1810.01473 [hep-ex]]

87. A. M. Sirunyan et al. [CMS Collaboration], “Search for new physics in final states with asingle photon and missing transverse momentum in proton-proton collisions at

√s = 13 TeV,”

JHEP 1902, 074 (2019) [47 pages]doi:10.1007/JHEP02(2019)074 [arXiv:1810.00196 [hep-ex]]

88. A. M. Sirunyan et al. [CMS Collaboration], “Combined measurements of Higgs boson couplingsin protonproton collisions at

√s = 13 TeV,” Eur. Phys. J. C 79, no. 5, 421 (2019) [67 pages]

doi:10.1140/epjc/s10052-019-6909-y [arXiv:1809.10733 [hep-ex]]

89. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of exclusive Υ photoproductionfrom protons in pPb collisions at

√sNN = 5.02 TeV,” Eur. Phys. J. C 79, no. 3, 277 (2019)

[36 pages]doi:10.1140/epjc/s10052-019-6774-8 [arXiv:1809.11080 [hep-ex]]

90. A. M. Sirunyan et al. [CMS Collaboration], “Search for single production of vector-like quarksdecaying to a top quark and a W boson in proton-proton collisions at

√s = 13 TeV,” Eur.

Phys. J. C 79, 90 (2019) [41 pages]doi:10.1140/epjc/s10052-019-6556-3 [arXiv:1809.08597 [hep-ex]]

91. A. M. Sirunyan et al. [CMS Collaboration], “Jet Shapes of Isolated Photon-Tagged Jets inPb-Pb and pp Collisions at

√sNN = 5.02 TeV,” Phys. Rev. Lett. 122, no. 15, 152001 (2019)

[18 pages]doi:10.1103/PhysRevLett.122.152001 [arXiv:1809.08602 [hep-ex]]

92. A. M. Sirunyan et al. [CMS Collaboration], “Search for invisible decays of a Higgs bosonproduced through vector boson fusion in proton-proton collisions at

√s = 13 TeV,” Phys.

Lett. B 793, 520 (2019) [32 pages]doi:10.1016/j.physletb.2019.04.025 [arXiv:1809.05937 [hep-ex]]

93. A. M. Sirunyan et al. [CMS Collaboration], “Search for the associated production of the Higgsboson and a vector boson in proton-proton collisions at

√s = 13 TeV via Higgs boson decays

to τ leptons,” JHEP 1906, 093 (2019) [41 pages]doi:10.1007/JHEP06(2019)093 [arXiv:1809.03590 [hep-ex]]

94. A. M. Sirunyan et al. [CMS Collaboration], “Search for pair production of second-generationleptoquarks at

√s = 13 TeV,” Phys. Rev. D 99, no. 3, 032014 (2019) [26 pages]

doi:10.1103/PhysRevD.99.032014 [arXiv:1808.05082 [hep-ex]]

95. A. M. Sirunyan et al. [CMS Collaboration], “Search for an Lµ−Lτ gauge boson using Z→ 4µevents in proton-proton collisions at

√s = 13 TeV,” Phys. Lett. B 792, 345 (2019) [24 pages]

doi:10.1016/j.physletb.2019.01.072 [arXiv:1808.03684 [hep-ex]]

96. A. M. Sirunyan et al. [CMS Collaboration], “Search for heavy resonances decaying into twoHiggs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV,”JHEP 1901, 051 (2019) [38 pages]doi:10.1007/JHEP01(2019)051 [arXiv:1808.01365 [hep-ex]]

97. A. M. Sirunyan et al. [CMS Collaboration], “Search for production of Higgs boson pairs inthe four b quark final state using large-area jets in proton-proton collisions at

√s = 13 TeV,”

JHEP 1901, 040 (2019) [43 pages]doi:10.1007/JHEP01(2019)040 [arXiv:1808.01473 [hep-ex]]

98. A. M. Sirunyan et al. [CMS Collaboration], “Search for narrow Hγ resonances in proton-protoncollisions at

√s = 13 TeV,” Phys. Rev. Lett. 122, no. 8, 081804 (2019) [18 pages]

doi:10.1103/PhysRevLett.122.081804 [arXiv:1808.01257 [hep-ex]]

16

99. A. M. Sirunyan et al. [CMS Collaboration], “Search for a W’ boson decaying to a τ leptonand a neutrino in proton-proton collisions at

√s = 13 TeV,” Phys. Lett. B 792, 107 (2019)

[25 pages]doi:10.1016/j.physletb.2019.01.069 [arXiv:1807.11421 [hep-ex]]

100. A. M. Sirunyan et al. [CMS Collaboration], “Search for dark matter particles produced inassociation with a top quark pair at

√s = 13 TeV,” Phys. Rev. Lett. 122, no. 1, 011803

(2019) [19 pages]doi:10.1103/PhysRevLett.122.011803 [arXiv:1807.06522 [hep-ex]]

101. A. M. Sirunyan et al. [CMS Collaboration], “Search for the Higgs boson decaying to two muonsin proton-proton collisions at

√s = 13 TeV,” Phys. Rev. Lett. 122, no. 2, 021801 (2019) [18

pages]doi:10.1103/PhysRevLett.122.021801 [arXiv:1807.06325 [hep-ex]]

102. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of inclusive and differential Higgsboson production cross sections in the diphoton decay channel in proton-proton collisions at√s = 13 TeV,” JHEP 1901, 183 (2019) [49 pages]

doi:10.1007/JHEP01(2019)183 [arXiv:1807.03825 [hep-ex]]

103. A. M. Sirunyan et al. [CMS Collaboration], “Study of the underlying event in top quark pairproduction in pp collisions at 13 TeV,” Eur. Phys. J. C 79, no. 2, 123 (2019) [64 pages]doi:10.1140/epjc/s10052-019-6620-z [arXiv:1807.02810 [hep-ex]]

104. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of differential cross sections forinclusive isolated-photon and photon+jets production in proton-proton collisions at

√s = 13

TeV,” Eur. Phys. J. C 79, no. 1, 20 (2019) [39 pages]doi:10.1140/epjc/s10052-018-6482-9 [arXiv:1807.00782 [hep-ex]]

105. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of differential cross sections for Zboson pair production in association with jets at

√s = 8 and 13 TeV,” Phys. Lett. B 789, 19

(2019) [26 pages]doi:10.1016/j.physletb.2018.11.007 [arXiv:1806.11073 [hep-ex]]

106. A. M. Sirunyan et al. [CMS Collaboration], “Search for heavy Majorana neutrinos in same-sign dilepton channels in proton-proton collisions at

√s = 13 TeV,” JHEP 1901, 122 (2019)

[51 pages]doi:10.1007/JHEP01(2019)122 [arXiv:1806.10905 [hep-ex]]

107. A. M. Sirunyan et al. [CMS Collaboration], “Search for supersymmetric partners of electronsand muons in proton-proton collisions at

√s = 13 TeV,” Phys. Lett. B 790, 140 (2019) [27

pages]doi:10.1016/j.physletb.2019.01.005 [arXiv:1806.05264 [hep-ex]]

108. A. M. Sirunyan et al. [CMS Collaboration], “Measurements of properties of the Higgs bosondecaying to a W boson pair in pp collisions at

√s = 13 TeV,” Phys. Lett. B 791, 96 (2019)

[34 pages]doi:10.1016/j.physletb.2018.12.073 [arXiv:1806.05246 [hep-ex]]

109. A. M. Sirunyan et al. [CMS Collaboration], “Search for Higgs boson pair production in theγγbb final state in pp collisions at

√s = 13 TeV,” Phys. Lett. B 788, 7 (2019) [30 pages]

doi:10.1016/j.physletb.2018.10.056 [arXiv:1806.00408 [hep-ex]]

110. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of nuclear modification factors ofΥ(1S), Υ(2S), and Υ(3S) mesons in PbPb collisions at

√sNN

= 5.02 TeV,” Phys. Lett. B 790,270 (2019) [24 pages]doi:10.1016/j.physletb.2019.01.006 [arXiv:1805.09215 [hep-ex]]

111. A. M. Sirunyan et al. [CMS Collaboration], “Measurement of prompt ψ(2S) production crosssections in proton-lead and proton-proton collisions at

√sNN

= 5.02 TeV,” Phys. Lett. B 790,509 (2019) [24 pages]doi:10.1016/j.physletb.2019.01.058 [arXiv:1805.02248 [hep-ex]]

17

112. A. M. Sirunyan et al. [CMS Collaboration], “Search for ttH production in the H→ bb decaychannel with leptonic tt decays in proton-proton collisions at

√s = 13 TeV,” JHEP 1903, 026

(2019) [59 pages]doi:10.1007/JHEP03(2019)026 [arXiv:1804.03682 [hep-ex]]

113. A. M. Sirunyan et al. [CMS Collaboration], “Search for a new scalar resonance decaying toa pair of Z bosons in proton-proton collisions at

√s = 13 TeV,” JHEP 1806, 127 (2018)

Erratum: [JHEP 1903, 128 (2019)] [50 pages]doi:10.1007/JHEP06(2018)127,10.1007/JHEP03(2019)128 [arXiv:1804.01939 [hep-ex]]

114. A. M. Sirunyan et al. [CMS Collaboration], “Non-Gaussian elliptic-flow fluctuations in PbPbcollisions at

√sNN

= 5.02 TeV,” Phys. Lett. B 789, 643 (2019) [23 pages]doi:10.1016/j.physletb.2018.11.063 [arXiv:1711.05594 [nucl-ex]]

115. S. Chatrchyan et al. [CMS Collaboration], “Observation of sequential Upsilon suppression inPbPb collisions,” Phys. Rev. Lett. 109, 222301 (2012) Erratum: [Phys. Rev. Lett. 120, no.19, 199903 (2018)] [25 pages]doi:10.1103/PhysRevLett.109.222301,10.1103/PhysRevLett.120.199903 [arXiv:1208.2826 [nucl-ex]]

116. V. Khachatryan et al. [CMS Collaboration], “Search for dark matter and unparticles producedin association with a Z boson in proton-proton collisions at

√s = 8??TeV,” Phys. Rev. D 93,

no. 5, 052011 (2016) Erratum: [Phys. Rev. D 97, no. 9, 099903 (2018)] [29 pages]doi:10.1103/PhysRevD.97.099903,10.1103/PhysRevD.93.052011 [arXiv:1511.09375 [hep-ex]]

117. A. M. Sirunyan et al. [CMS Collaboration], “Azimuthal anisotropy of charged particles withtransverse momentum up to 100 GeV/ c in PbPb collisions at

√sNN=5.02 TeV,” Phys. Lett.

B 776, 195 (2018) [22 pages]doi:10.1016/j.physletb.2017.11.041 [arXiv:1702.00630 [hep-ex]]

118. A. M. Sirunyan et al. [CMS Collaboration], “Measurements of tt cross sections in associationwith b jets and inclusive jets and their ratio using dilepton final states in pp collisions at

√s

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617. S. Chatrchyan et al. [CMS Collaboration], “Studies of azimuthal dihadron correlations inultra-central PbPb collisions at

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618. S. Chatrchyan et al. [CMS Collaboration], “Measurement of Higgs boson production andproperties in the WW decay channel with leptonic final states,” JHEP 1401, 096 (2014) [86pages][arXiv:1312.1129 [hep-ex]]

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624. S. Chatrchyan et al. [CMS Collaboration], “Search for supersymmetry in pp collisions at√s=8

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640. S. Chatrchyan et al. [CMS Collaboration], “Searches for new physics using the tt invariantmass distribution in pp collisions at

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675. S. Chatrchyan et al. [CMS Collaboration], “Search for a Higgs boson decaying into a b-quarkpair and produced in association with b quarks in proton-proton collisions at 7 TeV,” Phys.Lett. B 722, 207 (2013) [26 pages][arXiv:1302.2892 [hep-ex]]

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679. S. Chatrchyan et al. [CMS Collaboration], “Search for pair-produced dijet resonances in four-jet final states in pp collisions at

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684. S. Chatrchyan et al. [CMS Collaboration], “Search for physics beyond the standard model inevents with τ leptons, jets, and large transverse momentum imbalance in pp collisions at

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686. S. Chatrchyan et al. [CMS Collaboration], “Search for supersymmetry in events with opposite-sign dileptons and missing transverse energy using an artificial neural network,” Phys. Rev. D87, 072001 (2013) [21 pages][arXiv:1301.0916 [hep-ex]]

687. S. Chatrchyan et al. [CMS Collaboration], “Search for supersymmetry in pp collisions at√s = 7 TeV in events with a single lepton, jets, and missing transverse momentum,” Eur.

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689. S. Chatrchyan et al. [CMS Collaboration], “Measurements of differential jet cross sections inproton-proton collisions at

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695. S. Chatrchyan et al. [CMS Collaboration], “Search for heavy resonances in the W/Z-taggeddijet mass spectrum in pp collisions at 7 TeV,” Phys. Lett. B 723, 280 (2013) [29 pages][arXiv:1212.1910 [hep-ex]]

696. S. Chatrchyan et al. [CMS Collaboration], “Search for long-lived particles decaying to photonsand missing energy in proton-proton collisions at

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703. S. Chatrchyan et al. [CMS Collaboration], “Search in leptonic channels for heavy resonancesdecaying to long-lived neutral particles,” JHEP 1302, 085 (2013) [31 pages][arXiv:1211.2472 [hep-ex]]

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706. S. Chatrchyan et al. [CMS Collaboration], “Search for a non-standard-model Higgs bosondecaying to a pair of new light bosons in four-muon final states,” Phys. Lett. B 726, 564(2013) [23 pages][arXiv:1210.7619 [hep-ex]]

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711. S. Chatrchyan et al. [CMS Collaboration], “Observation of long-range near-side angular cor-relations in proton-lead collisions at the LHC,” Phys. Lett. B 718, 795 (2013) [20 pages][arXiv:1210.5482 [nucl-ex]]

712. S. Chatrchyan et al. [CMS Collaboration], “Search for excited leptons in pp collisions at√s = 7

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714. S. Chatrchyan et al. [CMS Collaboration], “Search for fractionally charged particles in ppcollisions at

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716. S. Chatrchyan et al. [CMS Collaboration], “Search for anomalous production of highly boostedZ bosons decaying to dimuons in pp collisions at

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717. S. Chatrchyan et al. [CMS Collaboration], “Search for a narrow spin-2 resonance decaying toa pair of Z vector bosons in the semileptonic final state,” Phys. Lett. B 718, 1208 (2013) [31pages][arXiv:1209.3807 [hep-ex]]

718. S. Chatrchyan et al. [CMS Collaboration], “Evidence for associated production of a single topquark and W boson in pp collisions at

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720. S. Chatrchyan et al. [CMS Collaboration], “Observation of a diffractive contribution to dijetproduction in proton-proton collisions at

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721. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the azimuthal anisotropy ofneutral pions in PbPb collisions at

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722. S. Chatrchyan et al. [CMS Collaboration], “Search for flavor changing neutral currents in topquark decays in pp collisions at 7 TeV,” Phys. Lett. B 718, 1252 (2013) [29 pages][arXiv:1208.0957 [hep-ex]]

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724. S. Chatrchyan et al. [CMS Collaboration], “Search for third-generation leptoquarks and scalarbottom quarks in pp collisions at

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725. S. Chatrchyan et al. [CMS Collaboration], “Observation of Z decays to four leptons with theCMS detector at the LHC,” JHEP 1212, 034 (2012) [27 pages][arXiv:1210.3844 [hep-ex]]

726. S. Chatrchyan et al. [CMS Collaboration], “Search for heavy neutrinos and WR bosons withright-handed couplings in a left-right symmetric model in pp collisions at

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727. S. Chatrchyan et al. [CMS Collaboration], “Search for heavy lepton partners of neutrinos inproton-proton collisions in the context of the type III seesaw mechanism,” Phys. Lett. B 718,348 (2012) [21 pages][arXiv:1210.1797 [hep-ex]]

728. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the relative prompt productionrate of χ(c2) and χ(c1) in pp collisions at

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729. S. Chatrchyan et al. [CMS Collaboration], “Search for electroweak production of charginosand neutralinos using leptonic final states in pp collisions at

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730. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the single-top-quark t-channelcross section in pp collisions at

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732. S. Chatrchyan et al. [CMS Collaboration], “Search for the standard model Higgs boson pro-duced in association with W and Z bosons in pp collisions at

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735. S. Chatrchyan et al. [CMS Collaboration], “Search for exclusive or semi-exclusive photonpair production and observation of exclusive and semi-exclusive electron pair production in ppcollisions at

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744. S. Chatrchyan et al. [CMS Collaboration], “Search for pair production of first- and second-generation scalar leptoquarks in pp collisions at

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750. S. Chatrchyan et al. [CMS Collaboration], “Search for new physics with long-lived particlesdecaying to photons and missing energy in pp collisions at

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756. S. Chatrchyan et al. [CMS Collaboration], “Measurement of jet fragmentation into chargedparticles in pp and PbPb collisions at

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762. S. Chatrchyan et al. [CMS Collaboration], “Search for a light pseudoscalar Higgs boson in thedimuon decay channel in pp collisions at

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763. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the electron charge asymmetry ininclusive W production in pp collisions at

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767. S. Chatrchyan et al. [CMS Collaboration], “Study of W boson production in PbPb and ppcollisions at

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768. S. Chatrchyan et al. [CMS Collaboration], “Search for a light charged Higgs boson in topquark decays in pp collisions at

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769. S. Chatrchyan et al. [CMS Collaboration], “Search for new physics in events with same-signdileptons and b-tagged jets in pp collisions at

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770. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Λb cross section and the Λbto Λb ratio with Λb → J/ψΛ decays in pp collisions at

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772. S. Chatrchyan et al. [CMS Collaboration], “Search for physics beyond the standard model inevents with a Z boson, jets, and missing transverse energy in pp collisions at

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774. S. Chatrchyan et al. [CMS Collaboration], “Search for anomalous tt production in the highly-boosted all-hadronic final state,” JHEP 1209, 029 (2012) [39 pages][arXiv:1204.2488 [hep-ex]]

775. S. Chatrchyan et al. [CMS Collaboration], “Azimuthal anisotropy of charged particles at hightransverse momenta in PbPb collisions at sqrtsNN = 2.76 TeV,” Phys. Rev. Lett. 109, 022301(2012) [27 pages][arXiv:1204.1850 [nucl-ex]]

776. S. Chatrchyan et al. [CMS Collaboration], “Search for Dark Matter and Large Extra Dimen-sions in pp Collisions Yielding a Photon and Missing Transverse Energy,” Phys. Rev. Lett.108, 261803 (2012) [27 pages][arXiv:1204.0821 [hep-ex]]

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780. S. Chatrchyan et al. [CMS Collaboration], “Measurement of isolated photon production in ppand PbPb collisions at

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781. S. Chatrchyan et al. [CMS Collaboration], “Search for heavy long-lived charged particles inpp collisions at

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782. S. Chatrchyan et al. [CMS Collaboration], “Observation of a new Ξb baryon,” Phys. Rev. Lett.108, 252002 (2012) [25 pages][arXiv:1204.5955 [hep-ex]]

783. S. Chatrchyan et al. [CMS Collaboration], “Search for anomalous production of multileptonevents in pp collisions at

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784. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the mass difference between topand antitop quarks,” JHEP 1206, 109 (2012) [33 pages][arXiv:1204.2807 [hep-ex]]

785. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Z/γ∗ + b-jet cross section inpp collisions at 7 TeV,” JHEP 1206, 126 (2012) [29 pages][arXiv:1204.1643 [hep-ex]]

786. S. Chatrchyan et al. [CMS Collaboration], “Search for heavy bottom-like quarks in 4.9 inversefemtobarns of pp collisions at

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787. S. Chatrchyan et al. [CMS Collaboration], “Search for B0s toµ

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788. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the cross section for productionof bbX, decaying to muons in pp collisions at

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789. S. Chatrchyan et al. [CMS Collaboration], “Search for microscopic black holes in pp collisionsat√s = 7 TeV,” JHEP 1204, 061 (2012) [33 pages]

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790. S. Chatrchyan et al. [CMS Collaboration], “Search for quark compositeness in dijet angulardistributions from pp collisions at

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791. S. Chatrchyan et al. [CMS Collaboration], “Jet momentum dependence of jet quenching inPbPb collisions at

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793. S. Chatrchyan et al. [CMS Collaboration], “Search for the standard model Higgs boson de-caying to bottom quarks in pp collisions at

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795. S. Chatrchyan et al. [CMS Collaboration], “Search for large extra dimensions in dimuon anddielectron events in pp collisions at

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796. S. Chatrchyan et al. [CMS Collaboration], “Search for the standard model Higgs boson in theH → ZZ → 2`2ν channel in pp collisions at

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797. S. Chatrchyan et al. [CMS Collaboration], “Search for the standard model Higgs boson in theH → ZZ → ``ττ decay channel in pp collisions at

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798. S. Chatrchyan et al. [CMS Collaboration], “Study of high-pT charged particle suppression inPbPb compared to pp collisions at

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801. S. Chatrchyan et al. [CMS Collaboration], “Search for the standard model Higgs boson de-caying into two photons in pp collisions at

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802. S. Chatrchyan et al. [CMS Collaboration], “Search for a Higgs boson in the decay channelH → ZZ∗ → qqbar`−`+ in pp collisions at

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803. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the inclusive production crosssections for forward jets and for dijet events with one forward and one central jet in pp collisionsat√s = 7 TeV,” JHEP 1206, 036 (2012) [37 pages]

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804. S. Chatrchyan et al. [CMS Collaboration], “Suppression of non-prompt J/ψ, prompt J/ψ, andΥ(1S) in PbPb collisions at

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805. S. Chatrchyan et al. [CMS Collaboration], “Centrality dependence of dihadron correlationsand azimuthal anisotropy harmonics in PbPb collisions at

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806. S. Chatrchyan et al. [CMS Collaboration], “Inclusive search for squarks and gluinos in ppcollisions at

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807. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at

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808. S. Chatrchyan et al. [CMS Collaboration], “Exclusive photon-photon production of muon pairsin proton-proton collisions at

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809. S. Chatrchyan et al. [CMS Collaboration], “J/ψ and ψ(2S) production in pp collisions at√s = 7 TeV,” JHEP 1202, 011 (2012) [39 pages]

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810. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Production Cross Section forPairs of Isolated Photons in pp collisions at

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811. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Rapidity and TransverseMomentum Distributions of Z Bosons in pp Collisions at

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812. S. Chatrchyan et al. [CMS Collaboration], “Jet Production Rates in Association with W andZ Bosons in pp Collisions at

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813. S. Chatrchyan et al. [CMS Collaboration], “Measurement of energy flow at large pseudora-pidities in pp collisions at

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814. S. Chatrchyan et al. [CMS Collaboration], “Forward Energy Flow, Central Charged-ParticleMultiplicities, and Pseudorapidity Gaps in W and Z Boson Events from pp Collisions at 7TeV,” Eur. Phys. J. C 72, 1839 (2012) [28 pages][arXiv:1110.0181 [hep-ex]]

815. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the weak mixing angle with theDrell-Yan process in proton-proton collisions at the LHC,” Phys. Rev. D 84, 112002 (2011)[41 pages][arXiv:1110.2682 [hep-ex]]

816. S. Chatrchyan et al. [CMS Collaboration], “Measurement of energy flow at large pseudora-pidities in pp collisions at

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817. S. Chatrchyan et al. [CMS Collaboration], “Search for a Vector-like Quark with Charge 2/3in t + Z Events from pp Collisions at

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818. S. Chatrchyan et al. [CMS Collaboration], “Search for Supersymmetry at the LHC in Eventswith Jets and Missing Transverse Energy,” Phys. Rev. Lett. 107, 221804 (2011) [16 pages][arXiv:1109.2352 [hep-ex]]

819. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the t t Production Cross Sectionin pp Collisions at 7 TeV in Lepton + Jets Events Using b-quark Jet Identification,” Phys.Rev. D 84, 092004 (2011) [39 pages][arXiv:1108.3773 [hep-ex]]

820. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Differential Cross Sectionfor Isolated Prompt Photon Production in pp Collisions at 7 TeV,” Phys. Rev. D 84, 052011(2011) [29 pages][arXiv:1108.2044 [hep-ex]]

821. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Drell-Yan Cross Section inpp Collisions at

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822. S. Chatrchyan et al. [CMS Collaboration], “Search for Bs and B to dimuon decays in ppcollisions at 7 TeV,” Phys. Rev. Lett. 107, 191802 (2011) [27 pages][arXiv:1107.5834 [hep-ex]]

823. S. Chatrchyan et al. [CMS Collaboration], “Search for Resonances in the Dijet Mass Spectrumfrom 7 TeV pp Collisions at CMS,” Phys. Lett. B 704, 123 (2011) [20 pages][arXiv:1107.4771 [hep-ex]]

824. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Inclusive W and Z ProductionCross Sections in pp Collisions at

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825. S. Chatrchyan et al. [CMS Collaboration], “Dependence on pseudorapidity and centrality ofcharged hadron production in PbPb collisions at a nucleon-nucleon centre-of-mass energy of2.76 TeV,” JHEP 1108, 141 (2011) [35 pages][arXiv:1107.4800 [nucl-ex]]

826. S. Chatrchyan et al. [CMS Collaboration], “Determination of Jet Energy Calibration andTransverse Momentum Resolution in CMS,” JINST 6, P11002 (2011) [67 pages][arXiv:1107.4277 [physics.ins-det]]

827. S. Chatrchyan et al. [CMS Collaboration], “Search for Three-Jet Resonances in pp Collisionsat√s = 7 TeV,” Phys. Rev. Lett. 107, 101801 (2011) [15 pages]

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828. S. Chatrchyan et al. [CMS Collaboration], “Search for supersymmetry in pp collisions at√s = 7 TeV in events with a single lepton, jets, and missing transverse momentum,” JHEP

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829. S. Chatrchyan et al. [CMS Collaboration], “A search for excited leptons in pp Collisions at√s = 7 TeV,” Phys. Lett. B 704, 143 (2011) [20 pages]

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830. S. Chatrchyan et al. [CMS Collaboration], “Inclusive search for squarks and gluinos in ppcollisions at

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831. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Underlying Event Activity atthe LHC with

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832. S. Chatrchyan et al. [CMS Collaboration], “Missing transverse energy performance of the CMSdetector,” JINST 6, P09001 (2011) [56 pages][arXiv:1106.5048 [physics.ins-det]]

833. S. Chatrchyan et al. [CMS Collaboration], “Search for New Physics with a Mono-Jet andMissing Transverse Energy in pp Collisions at

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834. S. Chatrchyan et al. [CMS Collaboration], “Search for New Physics with Jets and MissingTransverse Momentum in pp collisions at

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835. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Strange B Meson ProductionCross Section with J/ψφ Decays in pp Collisions at

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836. S. Chatrchyan et al. [CMS Collaboration], “Search for Supersymmetry in Events with b Jetsand Missing Transverse Momentum at the LHC,” JHEP 1107, 113 (2011) [24 pages][arXiv:1106.3272 [hep-ex]]

837. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the t-channel single top quarkproduction cross section in pp collisions at

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838. S. Chatrchyan et al. [CMS Collaboration], “Search for Light Resonances Decaying into Pairsof Muons as a Signal of New Physics,” JHEP 1107, 098 (2011) [28 pages][arXiv:1106.2375 [hep-ex]]

839. S. Chatrchyan et al. [CMS Collaboration], “Search for Same-Sign Top-Quark Pair Productionat√s = 7 TeV and Limits on Flavour Changing Neutral Currents in the Top Sector,” JHEP

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840. S. Chatrchyan et al. [CMS Collaboration], “Search for Physics Beyond the Standard ModelUsing Multilepton Signatures in pp Collisions at

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841. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Ratio of the 3-jet to 2-jetCross Sections in pp Collisions at

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842. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Inclusive Jet Cross Sectionin pp Collisions at

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843. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the tt production cross sectionand the top quark mass in the dilepton channel in pp collisions at

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844. S. Chatrchyan et al. [CMS Collaboration], “Search for First Generation Scalar Leptoquarksin the eνjj channel in pp collisions at

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845. S. Chatrchyan et al. [CMS Collaboration], “Indications of suppression of excited Υ states inPbPb collisions at

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846. S. Chatrchyan et al. [CMS Collaboration], “Search for supersymmetry in events with a lepton,a photon, and large missing transverse energy in pp collisions at

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847. S. Chatrchyan et al. [CMS Collaboration], “Measurement of Wγ and Zγ production in ppcollisions at

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848. S. Chatrchyan et al. [CMS Collaboration], “Long-range and short-range dihadron angularcorrelations in central PbPb collisions at a nucleon-nucleon center of mass energy of 2.76TeV,” JHEP 1107, 076 (2011) [30 pages][arXiv:1105.2438 [nucl-ex]]

849. S. Chatrchyan et al. [CMS Collaboration], “Charged particle transverse momentum spectrain pp collisions at

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850. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Polarization of W Bosonswith Large Transverse Momenta in W+Jets Events at the LHC,” Phys. Rev. Lett. 107, 021802(2011) [24 pages][arXiv:1104.3829 [hep-ex]]

851. S. Chatrchyan et al. [CMS Collaboration], “Search for new physics with same-sign isolateddilepton events with jets and missing transverse energy at the LHC,” JHEP 1106, 077 (2011)[40 pages][arXiv:1104.3168 [hep-ex]]

852. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the B0 production cross sectionin pp Collisions at

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853. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the differential dijet productioncross section in proton-proton collisions at

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854. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the Inclusive Z Cross Section viaDecays to Tau Pairs in pp Collisions at

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855. S. Chatrchyan et al. [CMS Collaboration], “Search for Neutral MSSM Higgs Bosons Decayingto Tau Pairs in pp Collisions at

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856. S. Chatrchyan et al. [CMS Collaboration], “Search for Large Extra Dimensions in the DiphotonFinal State at the Large Hadron Collider,” JHEP 1105, 085 (2011) [26 pages][arXiv:1103.4279 [hep-ex]]

857. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the lepton charge asymmetry ininclusive W production in pp collisions at

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858. S. Chatrchyan et al. [CMS Collaboration], “Search for Physics Beyond the Standard Model inOpposite-Sign Dilepton Events at

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859. S. Chatrchyan et al. [CMS Collaboration], “Search for Supersymmetry in pp Collisions at√s = 7 TeV in Events with Two Photons and Missing Transverse Energy,” Phys. Rev. Lett.

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860. S. Chatrchyan et al. [CMS Collaboration], “Search for Resonances in the Dilepton MassDistribution in pp Collisions at

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861. S. Chatrchyan et al. [CMS Collaboration], “Search for a W ′ boson decaying to a muon and aneutrino in pp collisions at

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862. S. Chatrchyan et al. [CMS Collaboration], “Measurement of W+W− Production and Searchfor the Higgs Boson in pp Collisions at

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963. T. A. Aaltonen et al. [CDF Collaboration], “Indirect measurement of sin2 θW (or MW ) usingµ+µ− pairs from γ∗/Z bosons produced in pp collisions at a center-of-momentum energy of1.96 TeV,” Phys. Rev. D 89, no. 7, 072005 (2014) [21 pages][arXiv:1402.2239 [hep-ex]]

964. T. A. Aaltonen et al. [CDF Collaboration], “Evidence for s-channel Single-Top-Quark Pro-duction in Events with one Charged Lepton and two Jets at CDF,” Phys. Rev. Lett. 112,231804 (2014) [8 pages][arXiv:1402.0484 [hep-ex]]

965. T. A. Aaltonen et al. [CDF Collaboration], “First Search for Exotic Z Boson Decays intoPhotons and Neutral Pions in Hadron Collisions,” Phys. Rev. Lett. 112, 111803 (2014) [8pages][arXiv:1311.3282 [hep-ex]]

966. T. A. Aaltonen et al. [CDF Collaboration], “Precise measurement of the W -boson mass withthe Collider Detector at Fermilab,” Phys. Rev. D 89, no. 7, 072003 (2014) [40 pages][arXiv:1311.0894 [hep-ex]]

967. T. A. Aaltonen et al. [CDF and D0 Collaborations], “Combination of measurements of thetop-quark pair production cross section from the Tevatron Collider,” Phys. Rev. D 89, no. 7,072001 (2014) [17 pages][arXiv:1309.7570 [hep-ex]]

968. T. A. Aaltonen et al. [CDF Collaboration], “Search for new physics in trilepton events andlimits on the associated chargino-neutralino production at CDF,” Phys. Rev. D 90, no. 1,012011 (2014) [9 pages][arXiv:1309.7509 [hep-ex]]

969. T. A. Aaltonen et al. [CDF Collaboration], “Study of orbitally excited B mesons and evidencefor a new Bπ resonance,” Phys. Rev. D 90, no. 1, 012013 (2014) [14 pages][arXiv:1309.5961 [hep-ex]]

970. T. Aaltonen et al. [CDF Collaboration], “Search for a dijet resonance in events with jets andmissing transverse energy in pp collisions at

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971. T. A. Aaltonen et al. [CDF Collaboration], “Observation of D0 −D0Mixing Using the CDF

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972. T. Aaltonen et al. [CDF Collaboration], “Production of K0S ,K

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973. T. A. Aaltonen et al. [CDF Collaboration], “Search for the production of ZW and ZZ bosonpairs decaying into charged leptons and jets in proton-antiproton collisions at

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974. T. A. Aaltonen et al. [CDF Collaboration], “A Direct Measurement of the Total Decay Widthof the Top Quark,” Phys. Rev. Lett. 111, 202001 (2013) [7 pages][arXiv:1308.4050 [hep-ex]]

975. T. A. Aaltonen et al. [CDF Collaboration], “Evidence for a bottom baryon resonance Λ∗b inCDF data,” Phys. Rev. D 88, 071101 (2013) [7 pages][arXiv:1308.1760 [hep-ex]]

976. T. A. Aaltonen et al. [CDF Collaboration], “Measurement of the leptonic asymmetry in tbevents produced in pbarp collisions at

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977. T. A. Aaltonen et al. [CDF and D0 Collaborations], “Combination of CDF and D0 W -BosonMass Measurements,” Phys. Rev. D 88, 052018 (2013) [11 pages][arXiv:1307.7627 [hep-ex]]

978. T. Aaltonen et al. [CDF Collaboration], “Indirect measurement of sin2θW (MW ) using e+e−

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979. T. Aaltonen et al. [CDF Collaboration], “A signature-based search for delayed photons inexclusive photon plus missing transverse energy events from pp collisions with

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980. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Differential Cross Sectiondσ/d(cosθt) for Top-Quark Pair Production in pp Collisions at

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981. T. Aaltonen et al. [CDF Collaboration], “Searches for the Higgs boson decaying to W+W− →`+ν`−ν with the CDF II detector,” Phys. Rev. D 88, 052012 (2013) [47 pages][arXiv:1306.0023 [hep-ex]]

982. T. Aaltonen et al. [CDF Collaboration], “Top-quark mass measurement in events with jetsand missing transverse energy using the full CDF data set,” Phys. Rev. D 88, 011101 (2013)[9 pages][arXiv:1305.3339 [hep-ex]]

983. T. Aaltonen et al. [CDF Collaboration], “Measurement of the top-quark pair production cross-section in events with two leptons and bottom-quark jets using the full CDF data set,” Phys.Rev. D 88, 091103 (2013) [7 pages][arXiv:1304.7961 [hep-ex]]

984. T. Aaltonen et al. [CDF Collaboration], “Exclusion of exotic top-like quarks with -4/3 electriccharge using jet-charge tagging in single-lepton tt events at CDF,” Phys. Rev. D 88, 032003(2013) [13 pages][arXiv:1304.4141 [hep-ex]]

985. T. Aaltonen et al. [CDF and D0 Collaborations], “Higgs Boson Studies at the Tevatron,”Phys. Rev. D 88, 052014 (2013) [27 pages][arXiv:1303.6346 [hep-ex]]

986. T. Aaltonen et al. [CDF Collaboration], “Measurement of R = B(t → Wb)/B(t → Wq) inTop–quark–pair Decays using Lepton+jets Events and the Full CDF Run II Data set,” Phys.Rev. D 87, 111101 (2013) [8 pages][arXiv:1303.6142 [hep-ex]]

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987. T. Aaltonen et al. [CDF Collaboration], “Measurement of the cross section for direct-photonproduction in association with a heavy quark in pp collisions at

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988. T. Aaltonen et al. [CDF Collaboration], “Search for pair-production of strongly-interactingparticles decaying to pairs of jets in pp collisions at

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989. T. Aaltonen et al. [CDF Collaboration], “Search for Supersymmetry with Like-Sign Lepton-Tau Events at CDF,” Phys. Rev. Lett. 110, 201802 (2013) [8 pages][arXiv:1302.4491 [hep-ex]]

990. T. Aaltonen et al. [CDF Collaboration], “Search for Bs → µ+µ− and Bd → µ+µ− decayswith the full CDF Run II data set,” Phys. Rev. D 87, 072003 (2013) [32 pages][arXiv:1301.7048 [hep-ex]]

991. T. Aaltonen et al. [CDF Collaboration], “Combination of searches for the Higgs boson usingthe full CDF data set,” Phys. Rev. D 88, 052013 (2013) [30 pages][arXiv:1301.6668 [hep-ex]]

992. T. Aaltonen et al. [CDF Collaboration], “Updated search for the standard model Higgs bosonin events with jets and missing transverse energy using the full CDF data set,” Phys. Rev. D87, 052008 (2013) [13 pages][arXiv:1301.4440 [hep-ex]]

993. T. Aaltonen et al. [CDF Collaboration], “Measurement of the cross section for prompt isolateddiphoton production using the full CDF Run II data sample,” Phys. Rev. Lett. 110, no. 10,101801 (2013) [55 pages][arXiv:1212.4204 [hep-ex]]

994. T. Aaltonen et al. [CDF Collaboration], “Search for a two-Higgs-boson doublet using a simpli-fied model in pp collisions at

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995. T. Aaltonen et al. [CDF Collaboration], “Search for Resonant tt Production in the Semi-leptonic Decay Mode Using the Full CDF Data Set,” Phys. Rev. Lett. 110, 121802 (2013) [8pages][arXiv:1211.5363 [hep-ex]]

996. T. Aaltonen et al. [CDF Collaboration], “Measurement of W -Boson Polarization in Top-quarkDecay using the Full CDF Run II Data Set,” Phys. Rev. D 87, 031104 (2013) [8 pages][arXiv:1211.4523 [hep-ex]]

997. T. Aaltonen et al. [CDF Collaboration], “Measurement of the top quark forward-backwardproduction asymmetry and its dependence on event kinematic properties,” Phys. Rev. D 87,092002 (2013) [23 pages][arXiv:1211.1003 [hep-ex]]

998. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Mass Difference Between Topand Anti-top Quarks at CDF,” Phys. Rev. D 87, 052013 (2013) [7 pages][arXiv:1210.6131 [hep-ex]]

999. T. Aaltonen et al. [CDF Collaboration], “Measurement of the B−c meson lifetime in the decayB−c → J/ψ π−,” Phys. Rev. D 87, 011101 (2013) [9 pages][arXiv:1210.2366 [hep-ex]]

1000. T. Aaltonen et al. [CDF Collaboration], “Observation of the Production of a W Boson inAssociation with a Single Charm Quark,” Phys. Rev. Lett. 110, no. 7, 071801 (2013) [7 pages][arXiv:1209.1921 [hep-ex]]

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1001. T. Aaltonen et al. [CDF Collaboration], “Search for the Higgs boson in the all-hadronic finalstate using the full CDF data set,” JHEP 1302, 004 (2013) [28 pages][arXiv:1208.6445 [hep-ex]]

1002. T. Aaltonen et al. [CDF Collaboration], “W boson polarization measurement in the tt dileptonchannel using the CDF II Detector,” Phys. Lett. B 722, 48 (2013) [7 pages][arXiv:1205.0354 [hep-ex]]

1003. S. Chatrchyan et al. [CMS Collaboration], “Forward-backward asymmetry of Drell-Yan leptonpairs in pp collisions at

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1004. S. Chatrchyan et al. [CMS Collaboration], “Search for new physics in events with opposite-signleptons, jets, and missing transverse energy in pp collisions at

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1005. S. Chatrchyan et al. [CMS Collaboration], “Studies of jet quenching using isolated-photon+jetcorrelations in PbPb and pp collisions at

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1006. S. Chatrchyan et al. [CMS Collaboration], “Measurement of the elliptic anisotropy of chargedparticles produced in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV,”Phys. Rev. C 87, 014902 (2013) [34 pages][arXiv:1204.1409 [nucl-ex]]

1007. T. Aaltonen et al. [CDF Collaboration], “Search for a heavy vector boson decaying to twogluons in pp collisions at

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1008. T. Aaltonen et al. [CDF Collaboration], “Measurements of the Top-quark Mass and the ttCross Section in the Hadronic τ+ Jets Decay Channel at

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1009. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Bottom-Strange Meson MixingPhase in the Full CDF Data Set,” Phys. Rev. Lett. 109, 171802 (2012) [8 pages][arXiv:1208.2967 [hep-ex]]

1010. T. Aaltonen et al. [CDF Collaboration], “Search for the standard model Higgs boson producedin association with top quarks using the full CDF data set,” Phys. Rev. Lett. 109, 181802(2012) [8 pages][arXiv:1208.2662 [hep-ex]]

1011. T. Aaltonen et al. [CDF Collaboration], “Novel inclusive search for the Higgs boson in thefour-lepton final state at CDF,” Phys. Rev. D 86, 072012 (2012) [8 pages][arXiv:1207.5016 [hep-ex]]

1012. T. Aaltonen et al. [CDF and D0 Collaborations], “Search for Neutral Higgs Bosons in Eventswith Multiple Bottom Quarks at the Tevatron,” Phys. Rev. D 86, 091101 (2012) [10 pages][arXiv:1207.2757 [hep-ex]]

1013. T. Aaltonen et al. [CDF and D0 Collaborations], “Combination of the top-quark mass mea-surements from the Tevatron collider,” Phys. Rev. D 86, 092003 (2012) [31 pages][arXiv:1207.1069 [hep-ex]]

1014. T. Aaltonen et al. [CDF Collaboration], “Search for Scalar Top Quark Production in ppCollisions at

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1015. T. Aaltonen et al. [CDF Collaboration], “Transverse momentum cross section of e+e− pairsin the Z-boson region from pp collisions at

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1016. T. Aaltonen et al. [CDF Collaboration], “Precision Top-Quark Mass Measurements at CDF,”Phys. Rev. Lett. 109, 152003 (2012) [7 pages][arXiv:1207.6758 [hep-ex]]

1017. T. Aaltonen et al. [CDF and D0 Collaborations], “Evidence for a particle produced in as-sociation with weak bosons and decaying to a bottom-antibottom quark pair in Higgs bosonsearches at the Tevatron,” Phys. Rev. Lett. 109, 071804 (2012) [11 pages][arXiv:1207.6436 [hep-ex]]

1018. T. Aaltonen et al. [CDF Collaboration], “Search for a Higgs boson in the diphoton final stateusing the full CDF data set from proton-antiproton collisions at

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1019. T. Aaltonen et al. [CDF Collaboration], “Measurement of the difference of CP–violatingasymmetries in D0 → K+K− and D0 → π+π− decays at CDF,” Phys. Rev. Lett. 109, 111801(2012) [7 pages][arXiv:1207.2158 [hep-ex]]

1020. T. Aaltonen et al. [CDF Collaboration], “Search for the standard model Higgs boson decayingto a bb pair in events with no charged leptons and large missing transverse energy using thefull CDF data set,” Phys. Rev. Lett. 109, 111805 (2012) [8 pages][arXiv:1207.1711 [hep-ex]]

1021. T. Aaltonen et al. [CDF Collaboration], “Combined search for the standard model Higgsboson decaying to a bb pair using the full CDF data set,” Phys. Rev. Lett. 109, 111802 (2012)[8 pages][arXiv:1207.1707 [hep-ex]]

1022. T. Aaltonen et al. [CDF Collaboration], “Search for the standard model Higgs boson decayingto a bb pair in events with two oppositely-charged leptons using the full CDF data set,” Phys.Rev. Lett. 109, 111803 (2012) [8 pages][arXiv:1207.1704 [hep-ex]]

1023. T. Aaltonen et al. [CDF Collaboration], “Search for the standard model Higgs boson decayingto a bb pair in events with one charged lepton and large missing transverse energy using thefull CDF data set,” Phys. Rev. Lett. 109, 111804 (2012) [8 pages][arXiv:1207.1703 [hep-ex]]

1024. T. Aaltonen et al. [CDF Collaboration], “Measurement of CP-violation asymmetries in D0 →KSπ

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1025. T. Aaltonen et al. [CDF Collaboration], “Search for the standard model Higgs boson producedin association with a W± boson with 7.5 fb−1 integrated luminosity at CDF,” Phys. Rev. D86, 032011 (2012) [14 pages][arXiv:1206.5063 [hep-ex]]

1026. T. Aaltonen et al. [CDF Collaboration], “Diffractive Dijet Production in pp Collisions at√s = 1.96 TeV,” Phys. Rev. D 86, 032009 (2012) [22 pages]

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1027. T. Aaltonen et al. [CDF Collaboration], “Measurement of B0s → D

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1029. T. Aaltonen et al. [CDF Collaboration], “Search for a heavy particle decaying to a top quarkand a light quark in pp collisions at

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1030. T. Aaltonen et al. [CDF Collaboration], “A Search for dark matter in events with one jet andmissing transverse energy in pp collisions at

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1031. T. Aaltonen et al. [CDF Collaboration], “Precise measurement of the W -boson mass with theCDF II detector,” Phys. Rev. Lett. 108, 151803 (2012) [4 pages][arXiv:1203.0275 [hep-ex]]

1032. T. Aaltonen et al. [CDF Collaboration], “Measurement of the WZ Cross Section and TripleGauge Couplings in pp Collisions at

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1033. T. Aaltonen et al. [CDF Collaboration], “Search for a dark matter candidate produced inassociation with a single top quark in pp collisions at

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1034. T. Aaltonen et al. [CDF and D0 Collaborations], “Combination of CDF and D0 measurementsof the W boson helicity in top quark decays,” Phys. Rev. D 85, 071106 (2012) [11 pages][arXiv:1202.5272 [hep-ex]]

1035. T. Aaltonen et al. [CDF Collaboration], “Search for anomalous production of multiple leptonsin association with W and Z bosons at CDF,” Phys. Rev. D 85, 092001 (2012) [17 pages][arXiv:1202.1260 [hep-ex]]

1036. T. Aaltonen et al. [CDF Collaboration], “Search for a low mass Standard Model Higgs bosonin the τ − τ decay channel in pp collisions at

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1037. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Top Quark Mass in the All-Hadronic Mode at CDF,” Phys. Lett. B 714, 24 (2012) [8 pages][arXiv:1112.4891 [hep-ex]]

1038. T. Aaltonen et al. [CDF Collaboration], “Search for Standard Model Higgs Boson Productionin Association with a W Boson Using a Matrix Element Technique at CDF in pp Collisions at√s = 1.96 TeV,” Phys. Rev. D 85, 072001 (2012) [29 pages]

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1039. T. Aaltonen et al. [CDF Collaboration], “Measurement of the branching fraction B(Λ0b →

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1040. T. Aaltonen et al. [CDF Collaboration], “Measurement of the masses and widths of the bottombaryons Σ+−

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1041. T. Aaltonen et al. [CDF Collaboration], “Measurement of ZZ production in leptonic finalstates at

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1042. T. Aaltonen et al. [CDF Collaboration], “Measurement of the CP-Violating Phase βJ/Ψφs in

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1043. T. Aaltonen et al. [CDF Collaboration], “Measurements of Angular Distributions of MuonsFrom Υ Meson Decays in pp Collisions at

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1044. T. Aaltonen et al. [CDF Collaboration], “Search for new phenomena in events with two Zbosons and missing transverse momentum in pp collisions at

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1045. T. Aaltonen et al. [CDF Collaboration], “Observation of Exclusive Gamma Gamma Produc-tion in pp Collisions at

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1046. T. Aaltonen et al. [CDF Collaboration], “Measurement of CP–violating asymmetries in D0 →π+π− and D0 → K+K− decays at CDF,” Phys. Rev. D 85, 012009 (2012) [29 pages][arXiv:1111.5023 [hep-ex]]

1047. T. Aaltonen et al. [CDF Collaboration], “An additional study of multi-muon events producedin pp collisions at

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1048. T. Aaltonen et al. [CDF Collaboration], “Search for high-mass resonances decaying into ZZin pp collisions at

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1049. T. Aaltonen et al. [CDF Collaboration], “Evidence for the charmless annihilation decay modeB0s → π+π−,” Phys. Rev. Lett. 108, 211803 (2012) [8 pages]

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1050. T. Aaltonen et al. [CDF Collaboration], “Search for a Higgs Boson in the Diphoton FinalState in pp Collisions at

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1051. T. Aaltonen et al. [CDF Collaboration], “Search for heavy metastable particles decaying tojet pairs in pp collisions at

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1052. T. Aaltonen et al. [CDF Collaboration], “Search for WZ + ZZ production with MET + jetswith b enhancement at

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1053. T. Aaltonen et al. [CDF Collaboration], “Measurements of the Angular Distributions in theDecays B → K(∗)µ+µ− at CDF,” Phys. Rev. Lett. 108, 081807 (2012) [7 pages][arXiv:1108.0695 [hep-ex]]

1054. T. Aaltonen et al. [CDF Collaboration], “Study of Substructure of High Transverse MomentumJets Produced in Proton-Antiproton Collisions at

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1055. T. Aaltonen et al. [CDF Collaboration], “Search for Higgs Bosons Produced in Associationwith b-quarks,” Phys. Rev. D 85, 032005 (2012) [20 pages][arXiv:1106.4782 [hep-ex]]

1056. T. Aaltonen et al. [CDF Collaboration], “Search for the Rare Radiative Decay: W → πγ inpp Collisions at

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1057. T. Aaltonen et al. [CDF Collaboration], “Production of Λ, Λ0 Ξ± and Ω± Hyperons in ppCollisions at

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1058. T. Aaltonen et al. [CDF Collaboration], “Top-quark mass measurement using events withmissing transverse energy and jets at CDF,” Phys. Rev. Lett. 107, 232002 (2011) [7 pages][arXiv:1109.1490 [hep-ex]]

1059. T. Aaltonen et al. [CDF Collaboration], “Measurements of branching fraction ratios and CP-asymmetries in suppressed B− → D(→ K+π−)K− and B− → D(→ K+π−)π− decays,” Phys.Rev. D 84, 091504 (2011) [8 pages][arXiv:1108.5765 [hep-ex]]

1060. T. Aaltonen et al. [CDF Collaboration], “Search for resonant production of tt decaying to jetsin pp collisions at

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1061. T. Aaltonen et al. [CDF Collaboration], “Measurement of the top-quark mass in the lep-ton+jets channel using a matrix element technique with the CDF II detector,” Phys. Rev. D84, 071105 (2011) [9 pages][arXiv:1108.1601 [hep-ex]]

1062. T. Aaltonen et al. [CDF Collaboration], “Search for new physics in high pT like-sign dileptonevents at CDF II,” Phys. Rev. Lett. 107, 181801 (2011) [7 pages][arXiv:1108.0101 [hep-ex]]

1063. T. Aaltonen et al. [CDF Collaboration], “A Search for resonant production of tt pairs in4.8 fb−1 of integrated luminosity of pp collisions at

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1064. T. Aaltonen et al. [CDF Collaboration], “Measurement of Polarization and Search for CP-Violation in B0

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1065. T. Aaltonen et al. [CDF Collaboration], “Search for a Heavy Top-Like Quark in pp Collisionsat√s = 1.96 TeV,” Phys. Rev. Lett. 107, 261801 (2011) [9 pages]

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1066. T. Aaltonen et al. [CDF Collaboration], “Observation of the Ξ0b Baryon,” Phys. Rev. Lett.

107, 102001 (2011) [16 pages][arXiv:1107.4015 [hep-ex]]

1067. T. Aaltonen et al. [CDF Collaboration], “Search for New T ′ Particles in Final States withLarge Jet Multiplicities and Missing Transverse Energy in ppbar Collisions at sqrt(s) = 1.96TeV,” Phys. Rev. Lett. 107, 191803 (2011) [7 pages][arXiv:1107.3574 [hep-ex]]

1068. T. Aaltonen et al. [CDF Collaboration], “Observation of the Baryonic Flavor-Changing Neu-tral Current Decay Λb → Λµ+µ−,” Phys. Rev. Lett. 107, 201802 (2011) [7 pages][arXiv:1107.3753 [hep-ex]]

1069. T. Aaltonen et al. [CDF Collaboration], “Search for Bs → µ+µ− and Bd → µ+µ− Decayswith CDF II,” Phys. Rev. Lett. 107, 239903 (2011) [7 pages][arXiv:1107.2304 [hep-ex]]

1070. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Cross Section for PromptIsolated Diphoton Production in pp Collisions at

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1071. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Cross Section for PromptIsolated Diphoton Production in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. D 84, 052006

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1072. T. Aaltonen et al. [CDF Collaboration], “Evidence for ttγ Production and Measurement ofσttγ/σtt,” Phys. Rev. D 84, 031104 (2011) [9 pages][arXiv:1106.3970 [hep-ex]]

1073. T. Aaltonen et al. [CDF Collaboration], “Measurement of branching ratio and B0s lifetime in

the decay B0s → J/ψf0(980) at CDF,” Phys. Rev. D 84, 052012 (2011) [14 pages]

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1074. T. Aaltonen et al. [CDF Collaboration], “Measurements of the properties of Λc(2595), Λc(2625),Σc(2455), and Σc(2520) baryons,” Phys. Rev. D 84, 012003 (2011) [17 pages][arXiv:1105.5995 [hep-ex]]

1075. T. Aaltonen et al. [CDF Collaboration], “Improved determination of the sample compositionof dimuon events produced in pp collisions at

√s = 1.96 TeV,” Eur. Phys. J. C 71, 1720 (2011)

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1076. T. Aaltonen et al. [CDF Collaboration], “First Search for Multijet Resonances in√s = 1.96

TeV pp Collisions,” Phys. Rev. Lett. 107, 042001 (2011) [6 pages][arXiv:1105.2815 [hep-ex]]

1077. T. Aaltonen et al. [CDF Collaboration], “Measurement of the tt production cross section inpp collisions at

√s = 1.96 TeV using events with large Missing ET and jets,” Phys. Rev. D

84, 032003 (2011) [12 pages][arXiv:1105.1806 [hep-ex]]

1078. T. Aaltonen et al. [CDF Collaboration], “Top quark mass measurement using the templatemethod at CDF,” Phys. Rev. D 83, 111101 (2011) [9 pages][arXiv:1105.0192 [hep-ex]]

1079. T. Aaltonen et al. [CDF Collaboration], “Search for a Very Light CP-Odd Higgs Boson inTop Quark Decays from p−p Collisions at 1.96 TeV,” Phys. Rev. Lett. 107, 031801 (2011) [7pages][arXiv:1104.5701 [hep-ex]]

1080. T. Aaltonen et al. [CDF Collaboration], “Invariant Mass Distribution of Jet Pairs Producedin Association with a W boson in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 106,

171801 (2011) [8 pages][arXiv:1104.0699 [hep-ex]]

1081. T. Aaltonen et al. [CDF Collaboration], “Measurements of Direct CP Violating Asymmetriesin Charmless Decays of Strange Bottom Mesons and Bottom Baryons,” Phys. Rev. Lett. 106,181802 (2011) [7 pages][arXiv:1103.5762 [hep-ex]]

1082. T. Aaltonen et al. [CDF Collaboration], “First Measurement of the Angular Coefficients ofDrell-Yan e+e− pairs in the Z Mass Region from pp Collisions at

√s = 1.96 TeV,” Phys. Rev.

Lett. 106, 241801 (2011) [7 pages][arXiv:1103.5699 [hep-ex]]

1083. T. Aaltonen et al. [CDF Collaboration], “Measurement of Event Shapes in Proton-AntiprotonCollisions at Center-of-Mass Energy 1.96 TeV,” Phys. Rev. D 83, 112007 (2011) [13 pages][arXiv:1103.5143 [hep-ex]]

1084. T. Aaltonen et al. [CDF Collaboration], “Search for New Dielectron Resonances and Randall-Sundrum Gravitons at the Collider Detector at Fermilab,” Phys. Rev. Lett. 107, 051801 (2011)[7 pages][arXiv:1103.4650 [hep-ex]]

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1085. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Top Pair Production CrossSection in the Lepton + Jets Channel Using a Jet Flavor Discriminant,” Phys. Rev. D 84,031101 (2011) [7 pages][arXiv:1103.4821 [hep-ex]]

1086. T. Aaltonen et al. [CDF Collaboration], “Measurement of the mass difference between t andt quarks,” Phys. Rev. Lett. 106, 152001 (2011) [7 pages][arXiv:1103.2782 [hep-ex]]

1087. T. Aaltonen et al. [CDF Collaboration], “Limits on Anomalous Trilinear Gauge Couplingsin Zγ Events from pp Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 107, 051802 (2011) [8

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1088. T. Aaltonen et al. [CDF Collaboration], “Search for Production of Heavy Particles Decayingto Top Quarks and Invisible Particles in pp collisions at

√s = 1.96 TeV,” Phys. Rev. Lett.

106, 191801 (2011) [7 pages][arXiv:1103.2482 [hep-ex]]

1089. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Bs Lifetime in Fully and Par-tially Reconstructed Bs → D−s (φπ−)X Decays in p − p Collisions at

√s = 1.96 TeV,” Phys.

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1090. T. Aaltonen et al. [CDF Collaboration], “Search for New Heavy Particles Decaying to ZZ →````, ``jj in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. D 83, 112008 (2011) [21 pages]

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1091. T. Aaltonen et al. [CDF Collaboration], “Observation of B0s → J/ψK∗0(892) and B0

s →J/ψK0

S Decays,” Phys. Rev. D 83, 052012 (2011) [15 pages][arXiv:1102.1961 [hep-ex]]

1092. T. Aaltonen et al. [The CDF Collaboration], “Search for the Higgs boson in the all-hadronicfinal state using the CDF II detector,” Phys. Rev. D 84, 052010 (2011) [12 pages][arXiv:1102.0024 [hep-ex]]

1093. T. Aaltonen et al. [The CDF Collaboration], “Search for heavy bottom-like quarks decayingto an electron or muon and jets in pp collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 106,

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1094. T. Aaltonen et al. [The CDF Collaboration], “Measurement of the Top Quark Mass in theLepton+Jets Channel Using the Lepton Transverse Momentum,” Phys. Lett. B 698, 371 (2011)[9 pages][arXiv:1101.4926 [hep-ex]]

1095. T. Aaltonen et al. [The CDF Collaboration], “Search for High Mass Resonances Decaying toMuon Pairs in

√s = 1.96 TeV pp Collisions,” Phys. Rev. Lett. 106, 121801 (2011) [7 pages]

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1096. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Forward-Backward Asymmetryin the B → K(∗)µ+µ− Decay and First Observation of the B0

s → φµ+µ− Decay,” Phys. Rev.Lett. 106, 161801 (2011) [7 pages][arXiv:1101.1028 [hep-ex]]

1097. T. Aaltonen et al. [CDF Collaboration], “Evidence for a Mass Dependent Forward-BackwardAsymmetry in Top Quark Pair Production,” Phys. Rev. D 83, 112003 (2011) [23 pages][arXiv:1101.0034 [hep-ex]]

1098. T. Aaltonen et al. [CDF Collaboration], “Search for a New Heavy Gauge Boson W ′ withElectron + missing ET Event Signature in pp collisions at

√s = 1.96 TeV,” Phys. Rev. D 83,

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1099. T. Aaltonen et al. [CDF Collaboration], “Measurement of tt Spin Correlation in pp CollisionsUsing the CDF II Detector at the Tevatron,” Phys. Rev. D 83, 031104 (2011) [8 pages][arXiv:1012.3093 [hep-ex]]

1100. T. Aaltonen et al. [CDF Collaboration], “Measurement of b hadron lifetimes in exclusivedecays containing a J/psi in pp collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 106, 121804

(2011) [8 pages][arXiv:1012.3138 [hep-ex]]

1101. T. Aaltonen et al. [CDF Collaboration], “Search for Randall-Sundrum Gravitons in the Dipho-ton Channel at CDF,” Phys. Rev. D 83, 011102 (2011) [8 pages][arXiv:1012.2795 [hep-ex]]

1102. T. Aaltonen et al. [CDF Collaboration], “Measurement of the tt Production Cross Sectionwith an in situ Calibration of b-jet Identification Efficiency,” Phys. Rev. D 83, 071102 (2011)[17 pages][arXiv:1007.4423 [hep-ex]]

1103. T. Aaltonen et al. [CDF Collaboration], “Measurement of the B− lifetime using a simulationfree approach for trigger bias correction,” Phys. Rev. D 83, 032008 (2011) [33 pages][arXiv:1004.4855 [hep-ex]]

1104. T. Aaltonen et al. [CDF Collaboration], “Comments and reply on: ’Study of multi-muonevents produced in interactions at

√s = 1.96 TeV’,” Eur. Phys. J. C68, 119-123 (2010). [5

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1105. T. Aaltonen et al. [CDF Collaboration], “Top Quark Mass Measurement in the Lepton + JetsChannel Using a Matrix Element Method and in situ Jet Energy Calibration,” Phys. Rev.Lett. 105, 252001 (2010). [7 pages][arXiv:1010.4582 [hep-ex]]

1106. T. Aaltonen et al. [CDF Collaboration], “Improved Search for a Higgs Boson Produced inAssociation with Z → `+`− in proton antiproton Collisions at

√s = 1.96 TeV,” Phys. Rev.

Lett. 105, 251802 (2010). [7 pages][arXiv:1009.3047 [hep-ex]]

1107. T. Aaltonen et al. [CDF Collaboration], “Search for the supersymmetric partner of the topquark in pp collisions at

√s = 1.96 TeV,” Phys. Rev. D82, 092001 (2010). [17 pages]

[arXiv:1009.0266 [hep-ex]]

1108. T. Aaltonen et al. [CDF Collaboration], “Updated Search for the Flavor-Changing Neutral-Current Decay D0 → µ+µ−,” Phys. Rev. D82, 091105 (2010). [8 pages][arXiv:1008.5077 [hep-ex]]

1109. T. Aaltonen et al. [CDF Collaboration], “Measurement of the WW + WZ Production CrossSection Using a Matrix Element Technique in Lepton + Jets Events,” Phys. Rev. D82, 112001(2010). [15 pages][arXiv:1008.4404 [hep-ex]]

1110. T. Aaltonen et al. [CDF Collaboration], “Direct Top-Quark Width Measurement CDF,” Phys.Rev. Lett. 105, 232003 (2010). [8 pages][arXiv:1008.3891 [hep-ex]]

1111. T. Aaltonen et al. [CDF Collaboration], “Diffractive W and Z Production at the FermilabTevatron,” Phys. Rev. D82, 112004 (2010). [10 pages][arXiv:1007.5048 [hep-ex]]

1112. T. Aaltonen et al. [CDF Collaboration], “Exclusion of an Exotic Top Quark with -4/3 ElectricCharge Using Soft Lepton Tagging,” Phys. Rev. Lett. 105, 101801 (2010). [7 pages][arXiv:1006.4597 [hep-ex]]

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1113. T. A. Aaltonen et al. [CDF Collaboration], “Measurement of dσ/dy of Drell-Yan e+e− pairs inthe Z Mass Region from pp Collisions at

√s = 1.96 TeV,” Phys. Lett. B692, 232-239 (2010).

[9 pages][arXiv:0908.3914 [hep-ex], arXiv:0908.3914]]

1114. T. Aaltonen et al. [ CDF and D0 Collaboration ], “Combined Tevatron upper limit on gg →H →W+W− and constraints on the Higgs boson mass in fourth-generation fermion models,”Phys. Rev. D82, 011102 (2010). [14 pages][arXiv:1005.3216 [hep-ex]]

1115. T. Aaltonen et al. [CDF Collaboration], “Search for the Production of Scalar Bottom Quarksin pp collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 105, 081802 (2010). [7 pages]

[arXiv:1005.3600 [hep-ex]]

1116. T. Aaltonen et al. [ The CDF Collaboration ], “Search for WW and WZ resonances decayingto electron, missing ET , and two jets in pp collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 104,

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1117. T. Aaltonen et al. [ The CDF Collaboration ], “Search for R-parity Violating Decays of τsneutrinos to eµ, µτ , and eτ Pairs in ppbar Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett.

105, 191801 (2010). [7 pages][arXiv:1004.3042 [hep-ex]]

1118. T. Aaltonen et al. [CDF Collaboration], “Measurement of Z gamma Production in pp Collisionsat√s = 1.96 TeV,” Phys. Rev. D82, 031103 (2010). [8 pages]

[arXiv:1004.1140 [hep-ex]]

1119. T. Aaltonen et al. [ The CDF Collaboration ], “Studying the Underlying Event in Drell-Yanand High Transverse Momentum Jet Production at the Tevatron,” Phys. Rev. D82, 034001(2010). [26 pages][arXiv:1003.3146 [Unknown]]

1120. T. Aaltonen et al. [ The CDF Collaboration ], “Measurement of W-Boson Polarization inTop-quark Decay in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 105, 042002 (2010). [8

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1121. T. Aaltonen et al. [CDF Collaboration], “Measurement of the tt Production Cross Sectionin pp Collisions at

√s = 1.96 TeV using Soft Electron b-Tagging,” Phys. Rev. D81, 092002

(2010). [18 pages][arXiv:1002.3783 [hep-ex]]

1122. T. Aaltonen et al. [ The CDF Collaboration ], “Measurement of the Top Pair ProductionCross Section in the Dilepton Decay Channel in pp Collisions at

√s = 1.96 TeV,” Phys. Rev.

D82, 052002 (2010). [24 pages][arXiv:1002.2919 [hep-ex]]

1123. T. Aaltonen et al. [ The CDF Collaboration ], “Measurement of the Top Quark Mass andpp→ tt Cross Section in the All-Hadronic Mode with the CDFII Detector,” Phys. Rev. D81,052011 (2010). [21 pages][arXiv:1002.0365 [hep-ex]]

1124. T. Aaltonen et al. [ CDF and D0 Collaboration ], “Combination of Tevatron searches forthe standard model Higgs boson in the W+W− decay mode,” Phys. Rev. Lett. 104, 061802(2010). [11 pages][arXiv:1001.4162 [hep-ex]]

1125. T. Aaltonen et al. [ The CDF Collaboration ], “Inclusive Search for Standard Model HiggsBoson Production in the WW Decay Channel using the CDF II Detector,” Phys. Rev. Lett.104, 061803 (2010). [8 pages][arXiv:1001.4468 [hep-ex]]

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1126. T. Aaltonen et al. [ The CDF Collaboration ], “Search for single top quark production in ppcollisions at

√s = 1.96 TeV in the missing transverse energy plus jets topology,” Phys. Rev.

D81, 072003 (2010). [25 pages][arXiv:1001.4577 [hep-ex]]

1127. T. Aaltonen et al. [CDF Collaboration], “Search for New Physics with a Dijet plus MissingTransverse Energy Signature in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 105, 131801

(2010). [7 pages][arXiv:0912.4691 [hep-ex]]

1128. T. Aaltonen et al. [CDF Collaboration], “Measurement of the W+W− Production CrossSection and Search for Anomalous WW gamma and WWZ Couplings in pp Collisions at√s = 1.96 TeV,” Phys. Rev. Lett. 104, 201801 (2010). [7 pages]

[arXiv:0912.4500 [hep-ex]]

1129. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Λ0b Lifetime in Λ0

b → Λ+c π−

Decays in pp Collisions at√s = 1.96 TeV,” Phys. Rev. Lett. 104, 102002 (2010). [8 pages]

[arXiv:0912.3566 [hep-ex]]

1130. T. Aaltonen et al. [CDF Collaboration], “A Study of the associated production of photonsand b-quark jets in pp collisions at

√s = 1.96 TeV,” Phys. Rev. D81, 052006 (2010). [8 pages]

[arXiv:0912.3453 [hep-ex]]

1131. T. Aaltonen et al. [CDF Collaboration], “Search for Technicolor Particles Produced in Asso-ciation with a W Boson at CDF,” Phys. Rev. Lett. 104, 111802 (2010). [9 pages][arXiv:0912.2059 [hep-ex]]

1132. T. Aaltonen et al. [CDF Collaboration], “Search for Pair Production of Supersymmetric TopQuarks in Dilepton Events from pp Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 104, 251801

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1133. T. Aaltonen et al. [CDF Collaboration], “Measurement of the WW + WZ Production CrossSection Using the Lepton+Jets Final State at CDF II,” Phys. Rev. Lett. 104, 101801 (2010).[7 pages][arXiv:0911.4449 [hep-ex]]

1134. T. Aaltonen et al. [CDF Collaboration], “A Search for the Higgs Boson Using Neural Networksin Events with Missing Energy and b-quark Jets in pp Collisions at

√s = 1.96 TeV,” Phys.

Rev. Lett. 104, 141801 (2010). [8 pages][arXiv:0911.3935 [hep-ex]]

1135. T. Aaltonen et al. [CDF Collaboration], “Search for New Color-Octet Vector Particle Decayingto tt in pp Collisions at

√s = 1.96 TeV,” Phys. Lett. B691, 183-190 (2010). [15 pages]

[arXiv:0911.3112 [hep-ex]]

1136. T. Aaltonen et al. [CDF Collaboration], “Top Quark Mass Measurement using mT2 in theDilepton Channel at CDF,” Phys. Rev. D81, 031102 (2010). [9 pages][arXiv:0911.2956 [hep-ex]]

1137. T. Aaltonen et al. [CDF Collaboration], “Measurements of branching fraction ratios and CPasymmetries in B± → DCPK

± decays in hadron collisions,” Phys. Rev. D81, 031105 (2010).[9 pages][arXiv:0911.0425 [hep-ex]]

1138. T. Aaltonen et al. [CDF Collaboration], “Search for Supersymmetry with Gauge-MediatedBreaking in Diphoton Events with Missing Transverse Energy at CDF II,” Phys. Rev. Lett.104, 011801 (2010). [7 pages][arXiv:0910.3606 [hep-ex]]

1139. T. Aaltonen et al. [CDF Collaboration], “Measurements of the top-quark mass using chargedparticle tracking,” Phys. Rev. D81, 032002 (2010). [22 pages][arXiv:0910.0969 [hep-ex]]

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1140. T. Aaltonen et al. [CDF Collaboration], “First Measurement of the b-jet Cross Section inEvents with a W Boson in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 104, 131801

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1141. T. Aaltonen et al. [CDF Collaboration], “Search for Anomalous Production of Events withTwo Photons and Additional Energetic Objects at CDF,” Phys. Rev. D82, 052005 (2010). [27pages][arXiv:0910.5170 [hep-ex]]

1142. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Inclusive Isolated PromptPhoton Cross Section in pp Collisions at

√s = 1.96 TeV using the CDF Detector,” Phys. Rev.

D80, 111106 (2009). [8 pages][arXiv:0910.3623 [hep-ex]]

1143. T. Aaltonen et al. [CDF Collaboration], “A Search for the Higgs Boson Produced in Associa-tion with Z → `+`− Using the Matrix Element Method at CDF II,” Phys. Rev. D80, 071101(2009). [7 pages][arXiv:0908.3534 [hep-ex]]

1144. T. Aaltonen et al. [CDF Collaboration], “Search for charged Higgs bosons in decays of topquarks in ppcollisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 103, 101803 (2009). [7 pages]

[arXiv:0907.1269 [hep-ex]]

1145. T. Aaltonen et al. [CDF Collaboration], “A Search for the Associated Production of theStandard-Model Higgs Boson in the All-Hadronic Channel,” Phys. Rev. Lett. 103, 221801(2009). [7 pages][arXiv:0907.0810 [hep-ex]]

1146. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Top Quark Mass Using theInvariant Mass of Lepton Pairs in Soft Muon b-tagged Events,” Phys. Rev. D80, 051104(2009). [9 pages][arXiv:0906.5371 [hep-ex]]

1147. T. Aaltonen et al. [CDF Collaboration], “Precision Measurement of the X(3872) Mass inJ/ψpi+pi− Decays,” Phys. Rev. Lett. 103, 152001 (2009). [7 pages][arXiv:0906.5218 [hep-ex]]

1148. T. Aaltonen et al. [CDF Collaboration], “Search for Higgs bosons predicted in two-Higgs-doublet models via decays to τ lepton pairs in 1.96-TeV pp collisions,” Phys. Rev. Lett. 103,201801 (2009). [7 pages][arXiv:0906.1014 [hep-ex]]

1149. T. Aaltonen et al. [CDF Collaboration], “Searching the Inclusive Lepton + Photon + MissingET + b-quark Signature for Radiative Top Quark Decay and Non-Standard-Model Processes,”Phys. Rev. D80, 011102 (2009). [9 pages][arXiv:0906.0518 [hep-ex]]

1150. T. Aaltonen et al. [CDF Collaboration], “First Observation of Vector Boson Pairs in a HadronicFinal State at the Tevatron Collider,” Phys. Rev. Lett. 103, 091803 (2009). [8 pages][arXiv:0905.4714 [hep-ex]]

1151. T. Aaltonen et al. [CDF Collaboration], “Observation of the Ω−b Baryon and Measurement ofthe Properties of the Ξ−b and Ω−b Baryons,” Phys. Rev. D80, 072003 (2009). [17 pages][arXiv:0905.3123 [hep-ex]]

1152. T. Aaltonen et al. [CDF Collaboration], “Production of ψ(2S) Mesons in ppCollisions at 1.96-TeV,” Phys. Rev. D80, 031103 (2009). [11 pages][arXiv:0905.1982 [hep-ex]]

1153. T. Aaltonen et al. [CDF Collaboration], “Search for a Fermiophobic Higgs Boson Decayinginto Diphotons in ppCollisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 103, 061803 (2009). [7

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1154. T. Aaltonen et al. [CDF Collaboration], “Search for the Neutral Current Top Quark Decayt→ Zc Using Ratio of Z-Boson + 4 Jets to W -Boson + 4 Jets Production,” Phys. Rev. D80,052001 (2009). [24 pages][arXiv:0905.0277 [hep-ex]]

1155. T. Aaltonen et al. [CDF Collaboration], “Search for Anomalous Production of Events with aPhoton, Jet, b-quark Jet, and Missing Transverse Energy,” Phys. Rev. D80, 052003 (2009).[20 pages][arXiv:0905.0231 [hep-ex]]

1156. T. Aaltonen et al. [CDF Collaboration], “Measurement of Particle Production and InclusiveDifferential Cross Sections in pp Collisions at

√s = 1.96 TeV,” Phys. Rev. D79, 112005 (2009).

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1157. T. Aaltonen et al. [CDF Collaboration], “A Measurement of the tt Cross Section in ppCollisionsat√s = 1.96 TeV using Dilepton Events with a Lepton plus Track Selection,” Phys. Rev. D79,

112007 (2009). [43 pages][arXiv:0903.5263 [hep-ex]]

1158. T. Aaltonen et al. [CDF Collaboration], “First Measurement of the tt Differential Cross Sectiondσ

dM(tt) in ppCollisions at√s = 1.96 TeV,” Phys. Rev. Lett. 102, 222003 (2009). [8 pages]

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1159. T. Aaltonen et al. [CDF Collaboration], “Search for Gluino-Mediated Sbottom Production inppCollisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 102, 221801 (2009). [7 pages]

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1160. T. Aaltonen et al. [CDF Collaboration], “Measurement of the b-Hadron Production CrossSection Using Decays to µ−D0X Final States in ppCollisions at

√s = 1.96 TeV,” Phys. Rev.

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1161. T. Aaltonen et al. [CDF Collaboration], “Evidence for a Narrow Near-Threshold Structure inthe J/ψφ Mass Spectrum in B+ → J/ψφK+ Decays,” Phys. Rev. Lett. 102, 242002 (2009).[7 pages][arXiv:0903.2229 [hep-ex]]

1162. T. Aaltonen et al. [CDF Collaboration], “Search for narrow resonances lighter than Upsilonmesons,” Eur. Phys. J. C62, 319-326 (2009). [9 pages][arXiv:0903.2060 [hep-ex]]

1163. T. Aaltonen et al. [CDF Collaboration], “Search for WW and WZ production in lepton plusjets final state at CDF,” Phys. Rev. D79, 112011 (2009). [9 pages][arXiv:0903.0814 [hep-ex]]

1164. T. Aaltonen et al. [CDF Collaboration], “Search for exclusive Z boson production and obser-vation of high mass pp → γγ → p + `` + p events in pp collisions at

√s = 1.96 TeV,” Phys.

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1165. T. Aaltonen et al. [CDF Collaboration], “Observation of exclusive charmonium productionand γγ → µ+µ− in pp collisions at

√s = 1.96 TeV,” Phys. Rev. Lett. 102, 242001 (2009). [7

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1166. T. Aaltonen et al. [CDF Collaboration], “Search for Long-Lived Massive Charged Particles in1.96 TeV pp Collisions,” Phys. Rev. Lett. 103, 021802 (2009). [16 pages][arXiv:0902.1266 [hep-ex]]

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1167. A. Abulencia et al. [CDF Collaboration], “eXtremely Fast Tracker trigger upgrade at CDF,”Nucl. Instrum. Meth. A598, 328-330 (2009). [3 pages]

1168. T. Aaltonen et al. [CDF Collaboration], “Measurement of the tt Production Cross Sectionin 2 fb−1 of pp Collisions at

√s = 1.96 TeV Using Lepton Plus Jets Events with Soft Muon

b-Tagging,” Phys. Rev. D79, 052007 (2009). [53 pages][arXiv:0901.4142 [hep-ex]]

1169. T. Aaltonen et al. [CDF Collaboration], “Search for the Decays B0s → e+mu− and B0

s → e+e−

in CDF Run II,” Phys. Rev. Lett. 102, 201801 (2009). [7 pages][arXiv:0901.3803 [hep-ex]]

1170. T. Aaltonen et al. [CDF Collaboration], “Measurement of the top quark mass at CDF usingthe ’neutrino φ weighting’ template method on a lepton plus isolated track sample,” Phys.Rev. D79, 072005 (2009). [17 pages][arXiv:0901.3773 [hep-ex]]

1171. T. Aaltonen et al. [CDF Collaboration], “Direct Measurement of the W Production ChargeAsymmetry in pp Collisions at

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1172. T. Aaltonen et al. [CDF Collaboration], “Top Quark Mass Measurement in the Lepton plusJets Channel Using a Modified Matrix Element Method,” Phys. Rev. D79, 072001 (2009). [46pages][arXiv:0812.4469 [hep-ex]]

1173. T. Aaltonen et al. [CDF Collaboration], “Measurement of Cross Sections for b Jet Productionin Events with a Z Boson in p− anti-p Collisions at

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1174. T. Aaltonen et al. [CDF Collaboration], “Observation of New Charmless Decays of BottomHadrons,” Phys. Rev. Lett. 103, 031801 (2009). [8 pages][arXiv:0812.4271 [hep-ex]]

1175. T. Aaltonen et al. [CDF Collaboration], “Search for new particles decaying into dijets inproton-antiproton collisions at

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1176. T. Aaltonen et al. [CDF Collaboration], Phys. Rev. Lett. 102, 151801 (2009). [8 pages][arXiv:0812.3400 [hep-ex]]

1177. T. Aaltonen et al. [CDF Collaboration], “Measurement of the kT Distribution of Particles inJets Produced in pp Collisions at

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1178. T. Aaltonen et al. [CDF Collaboration], “Inclusive Search for Squark and Gluino Productionin pp Collisions at

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1179. T. Aaltonen et al. [CDF Collaboration], “Top Quark Mass Measurement in the tt All HadronicChannel using a Matrix Element Technique in pp Collisions at

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1180. T. Aaltonen et al. [CDF Collaboration], “Measurement of W -Boson Helicity Fractions in Top-Quark Decays Using cosθ∗,” Phys. Lett. B674, 160-167 (2009). [17 pages][arXiv:0811.0344 [hep-ex]]

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1181. T. Aaltonen et al. [CDF Collaboration], “A Search for high-mass resonances decaying todimuons at CDF,” Phys. Rev. Lett. 102, 091805 (2009). [8 pages][arXiv:0811.0053 [hep-ex]]

1182. T. Aaltonen et al. [CDF Collaboration], “Search for new physics in the µµ+e/µ+ET channelwith a low-pT lepton threshold at the Collider Detector at Fermilab,” Phys. Rev. D79, 052004(2009). [17 pages][arXiv:0810.3522 [hep-ex]]

1183. T. Aaltonen et al. [CDF Collaboration], “First Measurement of the Ratio of Branching Frac-tions B(Λ0

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1184. T. Aaltonen et al. [CDF Collaboration], “Search for High-Mass e+ e- Resonances in pp Colli-sions at

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1185. T. Aaltonen et al. [CDF Collaboration], “Measurement of Resonance Parameters of OrbitallyExcited Narrow B0 Mesons,” Phys. Rev. Lett. 102, 102003 (2009). [7 pages][arXiv:0809.5007 [hep-ex]]

1186. T. Aaltonen et al. [CDF Collaboration], “Search for Maximal Flavor Violating Scalars inSame-Charge Lepton Pairs in pp Collisions at

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1187. T. Aaltonen et al. [CDF Collaboration], “First simultaneous measurement of the top quarkmass in the lepton + jets and dilepton channels at CDF,” Phys. Rev. D79, 092005 (2009). [24pages][arXiv:0809.4808 [hep-ex]]

1188. T. Aaltonen et al. [CDF Collaboration], “Search for a Higgs Boson Decaying to Two W Bosonsat CDF,” Phys. Rev. Lett. 102, 021802 (2009). [7 pages][arXiv:0809.3930 [hep-ex]]

1189. T. Aaltonen et al. [CDF Collaboration], “Global Search for New Physics with 2.0 fb−1 atCDF,” Phys. Rev. D79, 011101 (2009). [8 pages][arXiv:0809.3781 [hep-ex]]

1190. T. Aaltonen et al. [CDF Collaboration], “First observation of B0s → D±s K

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1191. T. Aaltonen et al. [CDF Collaboration], “First Direct Bound on the Total Width of the TopQuark in pp Collisions at

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1192. T. Aaltonen et al. [CDF Collaboration], “Measurement of the top quark mass with dileptonevents selected using neuroevolution at CDF,” Phys. Rev. Lett. 102, 152001 (2009). [7 pages][arXiv:0807.4652 [hep-ex]]

1193. T. Aaltonen et al. [CDF Collaboration], “Measurement of the fraction of tt production viagluon-gluon fusion in pp collisions at

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1194. T. Aaltonen et al. [CDF Collaboration], “Search for the Rare Decays B+ → µ+µ−K+, B0 →µ+µ−K∗0(892), and B0

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1195. T. Aaltonen et al. [CDF Collaboration], “Search for Hadronic Decays of W and Z Bosonsin Photon Events in pp Collisions at

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1196. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Single Top Quark ProductionCross Section at CDF,” Phys. Rev. Lett. 101, 252001 (2008). [7 pages][arXiv:0809.2581 [hep-ex]]

1197. T. Aaltonen et al. [CDF Collaboration], “Search for Supersymmetry in pp Collisions at√s =

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1198. T. Aaltonen et al. [ The CDF Collaboration ], “Search for Doubly Charged Higgs Bosons withLepton-Flavor-Violating Decays involving Tau Leptons,” Phys. Rev. Lett. 101, 121801 (2008).[7 pages][arXiv:0808.2161 [hep-ex]]

1199. T. Aaltonen et al. [CDF Collaboration], “Search for the Higgs boson produced with Z → `+`−

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1200. T. Aaltonen et al. [CDF Collaboration], “Search for large extra dimensions in final statescontaining one photon or jet and large missing transverse energy produced in pp collisions at√s = 1.96-TeV,” Phys. Rev. Lett. 101, 181602 (2008). [7 pages]

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1201. T. Aaltonen et al. [CDF Collaboration], “Measurement of the Inclusive Jet Cross Sectionat the Fermilab Tevatron pp Collider Using a Cone-Based Jet Algorithm,” Phys. Rev. D78,052006 (2008). [34 pages][arXiv:0807.2204 [hep-ex]]

1202. T. Aaltonen et al. [CDF Collaboration], “Forward-Backward Asymmetry in Top Quark Pro-duction in pp Collisions at sqrts = 1.96 TeV,” Phys. Rev. Lett. 101, 202001 (2008). [8 pages][arXiv:0806.2472 [hep-ex]]

1203. T. Aaltonen et al. [CDF Collaboration], “Measurement of b-jet Shapes in Inclusive Jet Pro-duction in pp Collisions at

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1204. T. Aaltonen et al. [CDF Collaboration], “Search for the Flavor Changing Neutral CurrentDecay t → Zq in pp Collisions at

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1205. T. Aaltonen et al. [CDF Collaboration], “Search for Heavy, Long-Lived Neutralinos that Decayto Photons at CDF II Using Photon Timing,” Phys. Rev. D78, 032015 (2008). [27 pages][arXiv:0804.1043 [hep-ex]]

1206. T. Aaltonen et al. [CDF Collaboration], “Search for Standard Model Higgs Boson Productionin Association with a W Boson at CDF,” Phys. Rev. D78, 032008 (2008). [35 pages][arXiv:0803.3493 [hep-ex]]

1207. T. Aaltonen et al. [CDF Collaboration], “Search for Pair Production of Scalar Top QuarksDecaying to a τ Lepton and a b Quark in pp Collisions at sqrts=1.96 TeV,” Phys. Rev. Lett.101, 071802 (2008). [8 pages][arXiv:0802.3887 [hep-ex]]

1208. T. Aaltonen et al. [CDF Collaboration], “Two-Particle Momentum Correlations in Jets Pro-duced in pp Collisions at

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1209. T. Aaltonen et al. [CDF Collaboration], “Search for the Higgs boson in events with missingtransverse energy and b quark jets produced in proton-antiproton collisions at

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1210. T. Aaltonen et al. [CDF Collaboration], “First Measurement of ZZ Production in panti-pCollisions at

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1211. T. Aaltonen et al. [CDF Collaboration], “Measurement of Ratios of Fragmentation Fractionsfor Bottom Hadrons in pp Collisions at

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1212. T. Aaltonen et al. [CDF Collaboration], “Search for New Heavy Particles Decaying to Z0Z0 →eeee in p - p Collisions at

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1213. T. Aaltonen et al. [CDF Collaboration], “First measurement of the fraction of top quark pairproduction through gluon-gluon fusion,” Phys. Rev. D78, 111101 (2008). [6 pages][arXiv:0712.3273 [hep-ex]]

1214. T. Aaltonen et al. [CDF Collaboration], “First Flavor-Tagged Determination of Bounds onMixing-Induced CP Violation in B0

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1215. T. Aaltonen et al. [CDF Collaboration], “Measurement of lifetime and decay-width differencein B0

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1216. T. Aaltonen et al. [CDF Collaboration], “Evidence for D0 − D0 mixing using the CDF IIDetector,” Phys. Rev. Lett. 100, 121802 (2008). [7 pages][arXiv:0712.1567 [hep-ex]]

1217. T. Aaltonen et al. [CDF Collaboration], “Search for B0s → µ+µ− and B0

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1218. T. Aaltonen et al. [CDF Collaboration], “Observation of the Decay B+ -(c) → J/ψπ± andMeasurement of the B+ -(c) Mass,” Phys. Rev. Lett. 100, 182002 (2008). [7 pages][arXiv:0712.1506 [hep-ex]]

1219. T. Aaltonen et al. [CDF Collaboration], “Model-Independent and Quasi-Model-IndependentSearch for New Physics at CDF,” Phys. Rev. D78, 012002 (2008). [39 pages][arXiv:0712.1311 [hep-ex]]

1220. T. Aaltonen et al. [CDF Collaboration], “Observation of Exclusive Dijet Production at theFermilab Tevatron p−p Collider,” Phys. Rev. D77, 052004 (2008). [27 pages][arXiv:0712.0604 [hep-ex]]

1221. T. Aaltonen et al. [CDF Collaboration], “Measurement of the cross section for W− bosonproduction in association with jets in ppbar collisions at

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1222. T. Aaltonen et al. [ CDF - Run II Collaboration ], “Measurement of inclusive jet cross-sectionsin Z/γ∗(→ e+e−) + jets production in pp collisions at

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1224. T. Aaltonen et al. [CDF Collaboration], “First measurement of the production of a W bosonin association with a single charm quark in pp collisions at

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1225. T. Aaltonen et al. [CDF Collaboration], “Limits on the production of narrow tt resonances inpp collisions at

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1226. T. Aaltonen et al. [CDF Collaboration], “Search for Standard Model Higgs Bosons Producedin Association with W Bosons,” Phys. Rev. Lett. 100, 041801 (2008). [17 pages][arXiv:0710.4363 [hep-ex]]

1227. T. Aaltonen et al. [CDF Collaboration], “Observation of orbitally excited Bs mesons,” Phys.Rev. Lett. 100, 082001 (2008). [7 pages][arXiv:0710.4199 [hep-ex]]

1228. T. Aaltonen et al. [CDF Collaboration], “A Direct measurement of the W boson width in ppcollisions at

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1229. T. Aaltonen et al. [CDF Collaboration], “Cross-section constrained top quark mass measure-ment from dilepton events at the Tevatron,” Phys. Rev. Lett. 100, 062005 (2008). [7 pages][arXiv:0710.4037 [hep-ex]]

1230. T. Aaltonen et al. [CDF Collaboration], “First Observation of the Decay B0s → D−s D

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1231. T. Aaltonen et al. [CDF Collaboration], “Measurement of correlated b−b production in p−pcollisions at

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1232. T. Aaltonen et al. [CDF Collaboration], “Search for resonant tt production in pp collisions at√s = 1.96-TeV,” Phys. Rev. Lett. 100, 231801 (2008). [7 pages]

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1233. T. Aaltonen et al. [CDF Collaboration], “First Run II Measurement of the W Boson Mass,”Phys. Rev. D77, 112001 (2008). [54 pages][arXiv:0708.3642 [hep-ex]]

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1235. T. Aaltonen et al. [CDF Collaboration], “Search for Third Generation Vector Leptoquarks inpp Collisions at

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1236. A. Abulencia et al. [CDF Collaboration], “Cross Section Measurements of High-pT DileptonFinal-State Processes Using a Global Fitting Method,” Phys. Rev. D78, 012003 (2008). [20pages][hep-ex/0612058]

1237. T. Aaltonen et al. [CDF Collaboration], “Search for Direct Pair Production of SupersymmetricTop and Supersymmetric Bottom Quarks in pp Collisions at

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1239. T. Aaltonen et al. [CDF Collaboration], “Search for exclusive γγ production in hadron-hadroncollisions,” Phys. Rev. Lett. 99, 242002 (2007). [7 pages][arXiv:0707.2374 [hep-ex]]

1240. T. Aaltonen et al. [CDF Collaboration], “Search for chargino-neutralino production in ppcollisions at

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1241. T. Aaltonen et al. [CDF Collaboration], “Search for a high-mass diphoton state and limits onRandall-Sundrum gravitons at CDF,” Phys. Rev. Lett. 99, 171801 (2007). [10 pages][arXiv:0707.2294 [hep-ex]]

1242. T. Aaltonen et al. [CDF Collaboration], “Observation and mass measurement of the baryonXi−b ,” Phys. Rev. Lett. 99, 052002 (2007). [8 pages][arXiv:0707.0589 [hep-ex]]

1243. T. Aaltonen et al. [CDF Collaboration], “First measurement of the W boson mass in run IIof the Tevatron,” Phys. Rev. Lett. 99, 151801 (2007). [7 pages][arXiv:0707.0085 [hep-ex]]

1244. T. Aaltonen et al. [CDF Collaboration], “First observation of heavy baryons Σb and Σ∗b ,”Phys. Rev. Lett. 99, 202001 (2007). [8 pages][arXiv:0706.3868 [hep-ex]]

1245. T. Aaltonen et al. [CDF Collaboration], “Measurement of the pp → tt production cross-section and the top quark mass at

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1246. T. Aaltonen et al. [CDF Collaboration], “Search for New Particles Leading to Z+ jets FinalStates in pp Collisions at

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1247. T. Aaltonen et al. [CDF Collaboration], “Limits on Anomalous Triple Gauge Couplings in ppCollisions at

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1248. T. Aaltonen et al. [CDF Collaboration], “Measurement of the top-quark mass using missingET + jets events with secondary vertex b−tagging at CDF II,” Phys. Rev. D75, 111103 (2007).[8 pages][arXiv:0705.1594 [hep-ex]]

1249. A. Abulencia et al. [CDF Collaboration], “Search for heavy, long-lived particles that decay tophotons at CDF II,” Phys. Rev. Lett. 99, 121801 (2007). [7 pages][arXiv:0704.0760 [hep-ex]]

1250. A. Abulencia et al. [CDF Collaboration], “Polarization of J/ψ and ψ2S mesons produced inpp collisions at

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1251. A. Abulencia et al. [CDF Collaboration], “Precise measurement of the top quark mass in thelepton+jets topology at CDF II,” Phys. Rev. Lett. 99, 182002 (2007). [7 pages][hep-ex/0703045]

1252. A. Abulencia et al. [CDF Collaboration], “Measurement of σχc2B(χc2 → J/ψγ)/σχc1B(χc1 →J/ψγ) in pp collisions at

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1253. A. Abulencia et al. [CDF Collaboration], “Inclusive search for new physics with like-signdilepton events in pp collisions at

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1254. A. Abulencia et al. [CDF Collaboration], “Measurement of σpp → Z · Br(Z → 2τ) in ppcollisions at

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1255. A. Abulencia et al. [CDF Collaboration], “First Measurement of the Ratio of Central-Electronto Forward-Electron W Partial Cross Sections in pp Collisions at

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1256. A. Abulencia et al. [CDF Collaboration], “Search for new physics in lepton + photon + Xevents with 929 pb(−1) of pp collisions at

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1257. A. Abulencia et al. [CDF Collaboration], “Observation of WZ Production,” Phys. Rev. Lett.98, 161801 (2007). [7 pages][hep-ex/0702027 [HEP-EX]]

1258. A. Abulencia et al. [ CDF - Run II Collaboration ], “Measurement of the Inclusive Jet CrossSection using the kT algorithm inpp Collisions at

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1259. A. Abulencia et al. [CDF Collaboration], “Search for anomalous production of multi-leptonevents in pp collisions at

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1260. A. Abulencia et al. [CDF Collaboration], “Search for Exotic S=-2 Baryons in proton-antiprotonCollisions at

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1261. A. Abulencia et al. [ CDF - Run II Collaboration ], “Measurement of the Top Quark Mass inppCollisions at

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1262. A. Abulencia et al. [ CDF - Run II Collaboration ], “Precision measurement of the top quarkmass from dilepton events at CDF II,” Phys. Rev. D75, 031105 (2007). [7 pages][hep-ex/0612060]

1263. A. Abulencia et al. [CDF Collaboration], “Analysis of the quantum numbers JPC of theX(3872),” Phys. Rev. Lett. 98, 132002 (2007). [7 pages][hep-ex/0612053]

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1266. A. Abulencia et al. [ CDF II Collaboration ], “Measurement of the Helicity Fractions of WBosons from Top Quark Decays using Fully Reconstructed tt Events with CDF II,” Phys. Rev.D75, 052001 (2007). [11 pages][hep-ex/0612011]

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1268. A. Abulencia et al. [CDF Collaboration], “Search for W -prime boson decaying to electron-neutrino pairs in pp collisions at

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1269. A. Abulencia et al. [CDF Collaboration], “Measurement of the Ratios of Branching Frac-tions B(B0

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1271. A. Abulencia et al. [CDF Collaboration], “Measurement of the Λ0b Lifetime in Λ0

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1272. A. Abulencia et al. [CDF Collaboration], “Search for V +A current in top quark decay in ppcollisions at

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1273. A. Abulencia et al. [CDF Collaboration], “Measurement of σ(Λ0b)/σ(B0) × BR(Λ0

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1278. A. Abulencia et al. [CDF Collaboration], “Search for excited and exotic muons in the µγdecay channel in pp collisions at

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1279. A. Abulencia et al. [ CDF - Run II Collaboration ], “Measurement of the B0s − B0

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1281. A. Abulencia et al. [CDF Collaboration], “Search for a neutral Higgs boson decaying to a Wboson pair in p antip collisions at

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1284. A. Abulencia et al. [CDF Collaboration], “Search for new physics in lepton + photon + Xevents with 305 pb−1 of pp collisions at

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1285. A. Abulencia et al. [CDF Collaboration], “Measurement of the ratio of branching fractionsB(D0 → K+π−)/B(D0→ K−π+) using the CDF II Detector,” Phys. Rev. D74, 031109(2006). [7 pages][hep-ex/0605027]

1286. A. Abulencia et al. [CDF Collaboration], “Search for Large Extra Dimensions in the Produc-tion of Jets and Missing Transverse Energy in pp Collisions at

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1287. A. Abulencia et al. [CDF Collaboration], “Measurement of the tt production cross sectionin pp collisions at

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1290. A. Abulencia et al. [CDF Collaboration], “Search for Z′ → e+e− using dielectron mass andangular distribution.,” Phys. Rev. Lett. 96, 211801 (2006). [7 pages][hep-ex/0602045]

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1294. A. Abulencia et al. [CDF Collaboration], “A search for scalar bottom quarks from gluinodecays in pp collisions at

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1297. A. Abulencia et al. [CDF Collaboration], “Search for anomalous semileptonic decay of heavyflavor hadrons produced in association with a W boson at CDF II,” Phys. Rev. D73, 051101(2006). [8 pages][hep-ex/0512065]

1298. A. Abulencia et al. [ CDF II Collaboration ], “Measurement of the inclusive jet cross sectionusing the kt algorithm in pp collisions at

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1299. A. Abulencia et al. [CDF Collaboration], “Search for H → bb produced in association withW bosons in pp collisions at

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1300. A. Abulencia et al. [CDF Collaboration], “Search for second-generation scalar leptoquarks inpp collisions at

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1301. A. Abulencia et al. [CDF Collaboration], “Measurement of the inclusive jet cross section in ppinteractions at

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1302. A. Abulencia et al. [CDF Collaboration], “Measurement of the top quark mass with thedynamical likelihood method using lepton plus jets events with b-tags in pp collisions at√s = 1.96-TeV.,” Phys. Rev. D73, 092002 (2006). [66 pages]

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1303. A. Abulencia et al. [CDF Collaboration], “Measurement of the helicity of W bosons in top-quark decays,” Phys. Rev. D73, 111103 (2006). [7 pages][hep-ex/0511023]

1304. A. Abulencia et al. [CDF Collaboration], “Search for charged Higgs bosons from top quarkdecays in pp collisions at

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1305. A. Abulencia et al. [CDF Collaboration], “A search for t→ tauνq in tt production.,” Phys.Lett. B639, 172-178 (2006). [7 pages][hep-ex/0510063]

1306. A. Abulencia et al. [CDF Collaboration], “Precision top quark mass measurement in the lepton+ jets topology in pp collisions at

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1307. A. Abulencia et al. [CDF Collaboration], “Top quark mass measurement using the templatemethod in the lepton + jets channel at CDF II,” Phys. Rev. D73, 032003 (2006). [77 pages][hep-ex/0510048]

1308. A. Abulencia et al. [CDF Collaboration], “Direct search for Dirac magnetic monopoles in ppcollisions at

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1309. A. Abulencia et al. [CDF Collaboration], “Search for neutral MSSM Higgs bosons decaying totau pairs in pp collisions at

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1310. D. E. Acosta et al. [CDF Collaboration], “Measurement of b hadron masses in exclusive J/ψdecays with the CDF detector,” Phys. Rev. Lett. 96, 202001 (2006). [7 pages][hep-ex/0508022]

1311. A. Abulencia et al. [CDF Collaboration], “Measurement of the ratios of branching fractions

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1312. D. E. Acosta et al. [CDF Collaboration], “Search for W and Z bosons in the reaction pp→2jets + γ at

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1313. A. Abulencia et al. [CDF Collaboration], “Evidence for the exclusive decay B±c → J/ψπ±

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1314. D. E. Acosta et al. [CDF Collaboration], “Measurement of the azimuthal angle distribution ofleptons from W boson decays as a function of the W transverse momentum in pp collisionsat√s = 1.8 TeV,” Phys. Rev. D73, 052002 (2006). [28 pages]

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1315. A. Abulencia et al. [CDF Collaboration], “Search for Bs → µ+µ− and Bd → µ+µ− decaysin pp collisions with CDF II,” Phys. Rev. Lett. 95, 221805 (2005). [7 pages][hep-ex/0508036]

1316. A. Abulencia et al. [CDF Collaboration], “Search for new high mass particles decaying tolepton pairs in pp collisions at

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1317. D. E. Acosta et al. [CDF Collaboration], “Search for Λb → pπ and Λb → pK decays in ppcollisions at

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1318. D. E. Acosta et al. [CDF Collaboration], “A search for supersymmetric Higgs bosons in thedi-tau decay mode in pp collisions at

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1319. D. E. Acosta et al. [CDF Collaboration], “Search for new physics using high mass τ pairsfrom 1.96 TeV pp collisions,” Phys. Rev. Lett. 95, 131801 (2005). [7 pages][hep-ex/0506034]

1320. D. E. Acosta et al. [CDF Collaboration], “Measurement of the tt production cross section inpp collisions at

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1321. D. E. Acosta et al. [CDF Collaboration], “Measurement of B(t→Wb)/B(t→Wq) at theCollider Detector at Fermilab,” Phys. Rev. Lett. 95, 102002 (2005). [7 pages][hep-ex/0505091]

1322. D. E. Acosta et al. [CDF Collaboration], “Study of jet shapes in inclusive jet production inpp collisions at

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1323. D. E. Acosta et al. [CDF Collaboration], “K0S and Λ0 production studies in pp collisions at√

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1324. D. E. Acosta et al. [CDF Collaboration], “Search for Higgs bosons decaying into bb andproduced in association with a vector boson in pp collisions at

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1325. D. E. Acosta et al. [CDF Collaboration], “Search for long-lived doubly-charged Higgs bosonsin pp collisions at

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1326. D. E. Acosta et al. [CDF Collaboration], “First evidence for B0s → φφ decay and measure-

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1327. D. E. Acosta et al. [CDF Collaboration], “Measurement of the moments of the hadronicinvariant mass distribution in semileptonic B decays,” Phys. Rev. D71, 051103 (2005). [9pages][hep-ex/0502003]

1328. D. E. Acosta et al. [CDF Collaboration], “Measurement of the W+W− production crosssection in pp collisions at

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1329. D. E. Acosta et al. [CDF Collaboration], “Measurement of the forward-backward chargeasymmetry from W → eν production in pp collisions at

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1330. D. E. Acosta et al. [CDF Collaboration], “Search for ZZ and ZW production in pp collisionsat√s = 1.96 TeV,” Phys. Rev. D71, 091105 (2005). [7 pages]

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1331. D. Acosta et al. [CDF Collaboration], “Measurement of the J/ψ meson and b−hadron pro-duction cross sections in pp collisions at

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1332. D. E. Acosta et al. [CDF Collaboration], “Measurement of the lifetime difference between Bs

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1333. D. E. Acosta et al. [CDF Collaboration], “Measurement of the cross section for promptdiphoton production in pp collisions at

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1334. D. E. Acosta et al. [CDF Collaboration], “Search for anomalous kinematics in tt dileptonevents at CDF II,” Phys. Rev. Lett. 95, 022001 (2005). [14 pages][hep-ex/0412042]

1335. D. E. Acosta et al. [CDF Collaboration], “Measurement of the W boson polarization in topdecay at CDF at

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1336. D. E. Acosta et al. [CDF Collaboration], “Measurement of the forward-backward chargeasymmetry of electron positron pairs in pp collisions at

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1337. D. E. Acosta et al. [CDF Collaboration], “Measurement of charged particle multiplicities ingluon and quark jets in pp collisions at

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1338. D. E. Acosta et al. [CDF Collaboration], “Search for scalar leptoquark pairs decaying to ννqqin pp collisions at

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1339. D. E. Acosta et al. [CDF Collaboration], “Search for electroweak single top quark productionin pp collisions at

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1340. D. E. Acosta et al. [CDF Collaboration], “Search for anomalous production of diphoton eventswith missing transverse energy at CDF and limits on gauge-mediated supersymmetry-breakingmodels,” Phys. Rev. D71, 031104 (2005). [9 pages][hep-ex/0410053]

1341. D. Acosta et al. [CDF Collaboration], “Measurement of the tt production cross section in ppcollisions at

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1342. D. E. Acosta et al. [CDF Collaboration], “Comparison of three-jet events in pp collisions at√s = 1.8 TeV to predictions from a next-to-leading order QCD calculation,” Phys. Rev.

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1343. D. E. Acosta et al. [CDF Collaboration], “Measurement of partial widths and search for directCP violation in D0 meson decays to K−K+ and π−π+,” Phys. Rev. Lett. 94, 122001 (2005).[7 pages][hep-ex/0504006]

1344. D. E. Acosta et al. [CDF Collaboration], “Search for excited and exotic electrons in the eγdecay channel in pp collisions at

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1345. D. E. Acosta et al. [ CDF II Collaboration ], “Measurement of Wγ and Zγ production in ppcollisions at

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1346. D. E. Acosta et al. [ CDF-II Collaboration ], “Measurement of the tt production cross sectionin pp collisions at

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1347. D. Acosta et al. [ CDF II Collaboration ], “First measurements of inclusive W and Z crosssections from Run II of the Tevatron collider,” Phys. Rev. Lett. 94, 091803 (2005). [8 pages][hep-ex/0406078]

1348. D. E. Acosta et al. [CDF Collaboration], “Search for doubly-charged Higgs bosons decayingto dileptons in pp collisions at

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1349. D. E. Acosta et al. [CDF Collaboration], “Inclusive search for anomalous production of highpT like-sign lepton pairs in pp collisions at

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1351. D. E. Acosta et al. [CDF Collaboration], “Direct photon cross section with conversions atCDF,” Phys. Rev. D70, 074008 (2004). [11 pages][hep-ex/0404022]

1352. D. E. Acosta et al. [CDF Collaboration], “The underlying event in hard interactions at theTevatron pp collider,” Phys. Rev. D70, 072002 (2004). [22 pages][hep-ex/0404004]

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1354. D. E. Acosta et al. [CDF Collaboration], “Search for B0s → µ+µ− and B0

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1355. D. E. Acosta et al. [ CDF II Collaboration ], “Observation of the narrow state X(3872) →J/ψπ+π− in pp collisions at

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1356. D. E. Acosta et al. [CDF Collaboration], “Measurement of the polar-angle distribution ofleptons from W boson decay as a function of the W transverse momentum in pp collisions at√s = 1.8 TeV,” Phys. Rev. D70, 032004 (2004). [43 pages]

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1358. D. E. Acosta et al. [CDF Collaboration], “Inclusive double pomeron exchange at the FermilabTevatron pp collider,” Phys. Rev. Lett. 93, 141601 (2004). [7 pages][hep-ex/0311023]

1359. D. Acosta et al. [CDF Collaboration], “Measurement of the average time-integrated mixingprobability of b-flavored hadrons produced at the Tevatron,” Phys. Rev. D69, 012002 (2004).[47 pages][hep-ex/0309030]

1360. D. E. Acosta et al. [CDF Collaboration], “Search for the flavor-changing neutral current decayD0 → µ+µ− in pp collisions at

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1361. D. E. Acosta et al. [ CDF II Collaboration ], “Measurement of the mass difference m(D+s )−

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1362. D. E. Acosta et al. [CDF Collaboration], “Measurement of prompt charm meson productioncross sections in pp collisions at

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1363. D. E. Acosta et al. [CDF Collaboration], “Search for associated production of Υ and vectorboson in pp collisions at

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1365. D. E. Acosta et al. [CDF Collaboration], “Search for pair production of scalar top quarksin R-parity violating decay modes in pp collisions at

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1366. D. E. Acosta et al. [ CDF and CDFII Collaborations ], “Central pseudorapidity gaps in eventswith a leading antiproton at the Fermilab Tevatron pp collider,” Phys. Rev. Lett. 91, 011802(2003). [7 pages][hep-ex/0303011]

1367. D. E. Acosta et al. [CDF Collaboration], “Search for the supersymmetric partner of the topquark in dilepton events from pp collisions at

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1368. D. E. Acosta et al. [CDF Collaboration], “Cross section for forward J/ψ production in ppcollisions at

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1369. D. E. Acosta et al. [CDF Collaboration], “Search for long-lived charged massive particles inpp collisions at

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1370. D. E. Acosta et al. [CDF Collaboration], “Search for a W ′ boson decaying to a top andbottom quark pair in 1.8 TeV pp collisions,” Phys. Rev. Lett. 90, 081802 (2003). [20 pages][hep-ex/0209030]

110