greg bock iwlc2010 19 october 2010
DESCRIPTION
Greg Bock IWLC2010 19 October 2010. Fermilab Program: Today and Tomorrow. Outline. Fermilab research program near and long term Emphasis on accelerator program and its evolution Further Emphasis Tevatron extension Project X Muon Collider feasibility study. - PowerPoint PPT PresentationTRANSCRIPT
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Greg BockIWLC2010
19 October 2010
Fermilab Program: Today and Tomorrow
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Outline
• Fermilab research program near and long term• Emphasis on accelerator program and its
evolution• Further Emphasis
Tevatron extension Project X Muon Collider feasibility study
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Fermilab Program at Three Frontiers Today
3
Hadron Colliders:
Tevatron
LHC
Neutrinos Supernova
Neutrinos
Dark Matter,
Dark Energy,
UHE Cosmic Rays
Accelerator and detector research and development at the 3 frontiers
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Present plan: energy frontier
4
TevatronLHC
LHC LHCILC, CLIC orMuon Collider
Now 2016
LHC UpgradesILC?
2013 2019 2022
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Present plan: intensity frontier
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MINOSMiniBooNEMINERvASeaQuest
NOvAMicroBooNEg-2?SeaQuest
Now 2016
LBNEMu2e
Project X+LBNEm, K, nuclear, …n Factory ??
2013 2019 2022
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Present plan: cosmic frontier
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Now 20162013 2019
DM: ~10 kgDE: SDSSP. Auger
DM: ~100 kgDE: DESP. AugerHolometer?
DM: ~1 tonDE: LSST WFIRST??BigBOSS??
DE: LSSTWFIRST??
2022
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Cosmic Frontier: Recent Results
COUPP (2010)
Young-Kee Kim, Report to FRA Board, Oct. 15, 2010
CDMS
Ultra high energycosmic rays
(Auger)
Dark Matter
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Fermilab Accelerator Complex
Operating Simultaneously
Tevatron
MINOS
MiniBooNE
MINERvA
Testbeam for Det.R&D
SeaQuest
Neutron Cancer Therapy
DØ
CDF
SCRF Test Facilities for Project X, ILC, Muon Collider,
Accelerator Research
Muon Cooling Test Facility
Main Injector
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Start of CMS Physics!!
CMS producing physics quickly
Fermilab serves as the U.S. hub for data analysis and operations LHC Physics Center
Computing facilities provide large resources to CMS and access to data
Remote Operations Center allows U.S. to engage in operations, shifts etc
Participate in Upgrades of both Accelerator and CMS
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LHC Instantaneous luminosity already > 1.5 x 1032 cm-2 s-1
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Energy Frontier: Recent Tevatron Results
• Tevatron continues to operate very well: ~25% of the favored region (114 – 185 GeV) now excluded
Exc
lud
ed
by
LE
P
Exc
lud
ed
by
Mto
p, M
W
95%
CL
Lim
it / S
M
Exc
lud
ed
by
LE
P
Exc
lud
ed
by
Mto
p, M
W
Exc
lude
d by
Te
vatr
onBest fit
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Tevatron extension (FY12 – FY14)
• A great short term opportunity for the Tevatron to get clearly into electroweak symmetry breaking territory
2s
3s
4s
5s
4sextension
present plan
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Tevatron-LHC: complementary
• All indirect measurements point to a light Higgs. It couples mostly to bb and the rate is robust in all models that are not highly contrived. If the Higgs is light we must measure the rate to bb.
• For the H bb, Tevatron is competitive through 2014 and in general will have higher signal to background than LHC
g
gb
b_
Tevatron LHC
_
_
_
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Tevatron extension: process
• Request from the community Tevatron experiments Letters to Steve Chu
~40 theorists 220 young scientists
• Very strong recommendations by Fermilab PAC PAC meeting in June Special PAC meeting in August
• DOE/NSF reconvened P5 on October 15-16• Special HEPAP meeting on October 26
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Laboratory’s position on Tevatron extension
• A great short term opportunity for the Tevatron to get clearly into electroweak symmetry breaking territory.
• However, we should not endanger the future. Additional resources (~$35M/year) into HEP in FY12-14 could mitigate. Even with additional funding, impact on NOvA cannot be mitigated. Most severe in 2015-2017 when the experiment would have ~50% of presently planned
• Weighing the pros and cons, we should try to extend Tevatron run and get solidly into electroweak symmetry braking territory if we get $35M/year in FY12-14.
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Interplay: LHC Intensity Frontier
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LHC
nothing
Lots
Intensity Frontier
Only handle on the next energy scale
Determine/verifystructure of new physics. Anything beyond?
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Intensity is key for neutrinos
• Recent Discoveries produced much excitement.
• Behave so different from other particles
• Possibly key to understand the matter-dominate Universe
• Unification
• Cosmic Connection
• This route like the energy path depends of what we find in the current generation of experiments
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17171717
m to e Conversion (mN eN)
for every incident proton 0.0025 m-’s are stopped in
the 17 0.2 mm Al target foils
Mu2E Project
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18 Target Mu2e sensitivity best in all scenarios
Loops Contact Terms
Mu2e can probe mass scales up to 104 TeV
SUSY
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A new (g-2) to uncertainty 0.14*10-11
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Model
UED
LHC
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Large effects in kaon decay rates
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d dW
Z
quarks
dd
WW
n
nn
n
s d quarkss
lepts
d
d d
squarks
dd
n
nn
n
s d squarkss
slepts
d
c
c
cc
SM: KLp0 n n
BSM: KLp0 n n
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The Quest for Electric Dipole Moments
+
-
+
-
-
+
T P
EDM Spin EDM Spin EDM Spin
A permanent EDM violates both time-reversal symmetry and parity
Neutron
Diamagnetic Atoms (Hg, Xe, Ra, Rn)
Paramagnetic Atoms (Tl, Fr)Molecules (PbO)
Quark EDM
Quark Chromo-EDM
Electron EDM
Physics beyond the Standard
Model:SUSY, Strings
…
To understand the origin of the symmetry violations, you need many experiments!
Guy Savard, ANL
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Intensity Frontier: Recent Results
MINOS: n vs anti- n MiniBooNE: n vs anti-n
neutrino behaviors = anti-neutrino behaviors ??more anti-neutrino data
n2 – n3 (MINOS – SuperK) n1 – n3 (CHOOZ – MINOS)
Best Dm232
q13 limits: comparable to the world best
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Neutrinossince 2013:
NOvA, MINERvAMicroBooNE
810 km 700 kW
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Intermediate Steps
NOvA (off-axis)MINERvASeaQuest
MicroBooNE (LAr TPC)
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Project X
Neutrino physicsMuon physicsKaon physics
Nuclear physics
Project X
Neutrino physicsMuon physicsKaon physics
Nuclear physics
RemoveAccelerators from Cockroft-Walton though Booster and Booster neutrino.
All the green onesincluding MuCOOL stay
“Ultimate Goal”multi MW beam
large detector (a few 100 kton)long distance (> 1,200 km)
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Project X provides:neutrinos
muonskaons nuclei
“simultaneously”
2 MW (60-120 GeV)1300 km
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Project X
Beam Power to 3 GeV program 2870 kWBeam Power to 8 GeV program 200 kW
Beam Power at 120 GeV 2200 kW
Design based on three families of 325 MHz Spoke resonators, two families of 650 MHz elliptical cavities, then 1300 MHz ILC cavities. Earliest construction start of 2015, operations in 2020. 3-8 GeV Linac is very similar to ILC. Same cavities, similar cryomodules.
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26Final Assembly
HTSVTS
String Assembly MP9 Clean RoomVTS
1st U.S. built ILC/PX Cryomodule 1st Dressed Cavity
Cavity tuning machine
New FNAL SRF infrastructure
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Fermilab
Tevatron
CERN
LHC Lepton Collider
(ILC, CLIC, Muon Collider)(energy decision)
Energy Frontier: Plan
Young-Kee Kim, Report to FRA Board, Oct. 15, 2010
SCRF: ILC R&D, Muon Collider, Project XHigh field magnets: LHC upgrades, Muon Collider
Fermilab:CMS / Machine
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Muon Collider
• Collider based on a secondary beam: we have experience basing colliders on antiprotons. For muons we must do it in 20 msec. The biggest advantages are: narrow energy spread (no beamstrahlung) and small physical footprint (no synchrotron radiation
• After a decade of steady progress on Muon Collider design and technology development, a new national U.S. organization (Muon Accelerator Program) has been put in place, led and hosted by Fermilab.MAP aims to deliver a Muon Collider Design feasibility Study within ~6 years.
• A parallel Physics and Detector study is also being launched. There appears to be very significant synergies with other lepton collider detector needs and challenges.
• There will be a Muon Collider meeting 27 June – 1st July 2011 (place to be determined) to build community awareness of the progress and R&D opportunities.
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l+l-→ Z’ →m+m-
Lucie Linssen, SPC, 15/6/2009
ENERGY SCANm+m-with ISR+BStr (Eichten)
e+e- with ISR
e+e- with ISR+BStr
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Muon Collider Schematic
Proton source: Example: upgraded PROJECT X (4 MW, 2±1 ns long bunches)
1021 muons per year that fit within the acceptance of an accelerator: eN=6000 mm e//N=25 mm
√s = 3 TeV Circumference = 4.5kmL = 3×1034 cm-2s-1m/bunch = 2x1012
s(p)/p = 0.1%eN = 25 mm, e//N=70 mmb* = 5mmRep Rate = 12Hz
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31 Sample Communication Talk3124
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