nuclear and hadron physics perspectives within infn paris, march 7, 2011 angela bracco
DESCRIPTION
Nuclear and Hadron Physics Perspectives within INFN Paris, March 7, 2011 Angela Bracco. ….. The 4 scientific lines. Line 2- 198 FTE: Phase transitions in nuclear matter (160 in Alice). Line 1 -149 FTE: Quarks and Hadron Dynamics (Jlab- LNF- GSI). CSN3 542 FTE. - PowerPoint PPT PresentationTRANSCRIPT
Nuclear and Hadron Physics Nuclear and Hadron Physics PerspectivesPerspectiveswithin INFNwithin INFN
Paris, March 7, 2011 Paris, March 7, 2011
Angela BraccoAngela Bracco
Nuclear and Hadron Physics Nuclear and Hadron Physics PerspectivesPerspectiveswithin INFNwithin INFN
Paris, March 7, 2011 Paris, March 7, 2011
Angela BraccoAngela Bracco
CSN3CSN3542 FTE542 FTECSN3CSN3
542 FTE542 FTE
Line 1 -149 FTE:Line 1 -149 FTE: Quarks and Hadron Dynamics(Jlab- LNF- GSI)
Line 2- 198 FTE:Line 2- 198 FTE:Phase transitions in nuclear matter (160 in Alice)
Line 3- 121 FTE: Line 3- 121 FTE: Nuclear Structure and reaction mechanisms(LNL-LNS)
Line 4- 71 FTE: Line 4- 71 FTE: Nuclear Astrophysicsand interdisciplinary research(LNGS-LNS
…….. The 4 scientific lines.. The 4 scientific lines
CSN3: Publications, presentations to conferences ….
In 2009In 2009:
240 Papers
486 Conference presentations
In 2009In 2009:
240 Papers
486 Conference presentations
Post doc 108Post doc 108
65 Doctoral students 65 Doctoral students
(16 doctoral thesis (16 doctoral thesis completed) completed)
27 Master thesis – 23 27 Master thesis – 23 thesis (3 years degree)thesis (3 years degree)
Post doc 108Post doc 108
65 Doctoral students 65 Doctoral students
(16 doctoral thesis (16 doctoral thesis completed) completed)
27 Master thesis – 23 27 Master thesis – 23 thesis (3 years degree)thesis (3 years degree)
Line 1:Line 1: hadron dynamics hadron dynamics
Linea 2 Linea 2 : Phase Transition: Phase Transition
Linea 3Linea 3 : Nuclear Structure : Nuclear Structure
Linea 4Linea 4 : Nuclear Astrophysics : Nuclear Astrophysics
Line 1:Line 1: hadron dynamics hadron dynamics
Linea 2 Linea 2 : Phase Transition: Phase Transition
Linea 3Linea 3 : Nuclear Structure : Nuclear Structure
Linea 4Linea 4 : Nuclear Astrophysics : Nuclear Astrophysics
698 Reserachers+ 99 Tech. 698 Reserachers+ 99 Tech.
542 FTE542 FTE0.0
10.0
20.0
30.0
40.0
50.0
Linea 1 Linea 2 Linea 3 Linea 4
27.5
36.9
22.4
13.1
31.9
18.1
42.1
7.9
Ripartizione delle pubblicazioni 2009nelle
linee di ricerca
FTE (%)
pubblicazioni (%)% FTE% FTE
% Pub% Pub
Line 1:Line 1: hadron dynamics hadron dynamics
Linea 2 Linea 2 : Phase Transition: Phase Transition
Linea 3Linea 3 : Nuclear Structure : Nuclear Structure
Linea 4Linea 4 : Nuclear Astrophysics : Nuclear Astrophysics
Line 1:Line 1: hadron dynamics hadron dynamics
Linea 2 Linea 2 : Phase Transition: Phase Transition
Linea 3Linea 3 : Nuclear Structure : Nuclear Structure
Linea 4Linea 4 : Nuclear Astrophysics : Nuclear Astrophysics
Distribution of fundings and of FTE in the reserach linesDistribution of fundings and of FTE in the reserach lines
0.0
10.0
20.0
30.0
40.0
50.0
Linea 1 Linea 2 Linea 3 Linea 4
27.5
36.9
22.4
13.1
24.2
43.1
21.7
11.0
Ripartizione dei finanziamenti e degli FTE fra le diverse linee di ricerca
FTE (%)
Finanziamenti 2009 (%)
0.0
10.0
20.0
30.0
40.0
50.0
Linea 1 Linea 2 Linea 3 Linea 4
27.5
36.9
22.4
13.1
24.2
43.1
21.7
11.0
Ripartizione dei finanziamenti e degli FTE fra le diverse linee di ricerca
FTE (%)
Finanziamenti 2009 (%)
LNF, JLAB, GSILNF, JLAB, GSI CERNCERN LNL-LNS-LNGSLNL-LNS-LNGS
27.5
36.8
22.4
13.111.0
21.7
43.1
24.2
Nuclear Physics Nuclear Physics 17 sections + 4 Labs17 sections + 4 Labs
Line 1:Line 1: hadron dynamics hadron dynamics
Linea 2 Linea 2 : Phase Transition: Phase Transition
Linea 3Linea 3 : Nuclear Structure : Nuclear Structure
Linea 4Linea 4 : Nuclear : Nuclear AstrophysicsAstrophysics
Line 1:Line 1: hadron dynamics hadron dynamics
Linea 2 Linea 2 : Phase Transition: Phase Transition
Linea 3Linea 3 : Nuclear Structure : Nuclear Structure
Linea 4Linea 4 : Nuclear : Nuclear AstrophysicsAstrophysics
Quarks and Hadron DynamicsQuarks and Hadron Dynamics
N
WN
N
S --
KK
Problem of the spin Problem of the spin Nucleon form factors -Nucleon form factors -Structure functions and GPD- Structure functions and GPD- (JLAB12)
Barionic resonaces and Barionic resonaces and Spectroscopy of mesons Spectroscopy of mesons (JLAB12- MAMBO-PAINUC) Ipernuclei and Ipernuclei and
Kaonic atoms Kaonic atoms (interaction (interaction ΛΛ-N e K--N e K-N) N) (SIDDHARTHA- FINUDA)
+ R&D for PANDA e PAX (antiprotons at FAIR)
BARIONIC RESONANCES 1.5 GeV -3 GeV BARIONIC RESONANCES 1.5 GeV -3 GeV MAMBO experiment
BGO ball(ex-GRAAL)mounted with a Spectrometerfor charged particles
Future experiments at Bonn with polarized beams and targets
Precise measurements of beam-helicity Precise measurements of beam-helicity asymmetry for double pion asymmetry for double pion photoproductions on protonphotoproductions on proton
New data from MAMI (PRL103,052002(2009)
Rigorous test for developments to extract resonance contributions
present data
th. prediction
previous data
hypernucleusmesonic decay
hypernucleusmesonic decay
pF ~ 270 MeV/cW
N
suppressed byPauli blocking
suppressed byPauli blocking
ΓT = ΓM + ΓNM
ΓM = Γπ0 + Γπ- ΓNM = Γn + Γp + Γ2
ΓT = ΓM + ΓNM
ΓM = Γπ0 + Γπ- ΓNM = Γn + Γp + Γ2
FINUDA
…….. .. ΛΛ decays in nuclei……. from FINUDA (LNF) decays in nuclei……. from FINUDA (LNF)
hypernucleusnon-mesonic decay
hypernucleusnon-mesonic decay
N
WN
N
SpN ~ 400 MeV/c
FINUDA
Decadimento non Decadimento non mesonicomesonico
Decadimento Decadimento mesonicomesonico
Kaonic atoms at LNF (Kaonic atoms at LNF (SIDDHARTA)SIDDHARTA)
For Kaonic deuteron more data with an improved set up and electronics are needed – proposed in the next yearsproposed in the next yearsComplementary experiments are made at JPARC
Measurement of the energy for the level 1s for the hydrogen kaonic atom
Kaonic Kaonic 44HeHePLB 681 (2009) 310
siddharta preliminarysiddharta preliminary
In agreement with theoryIn agreement with theory
PANDA
Straw Tube Tracker-LNFStraw Tube Tracker-LNF
TDR on TDR on SolenoidSolenoidContribution of Contribution of INFN was INFN was essential essential
Jet target Jet target developmentdevelopment
Attività di R&D Attività di R&D -Writing of TDR -Writing of TDR
Attivity on the micro-vertex detector Attivity on the micro-vertex detector
Simulation activity Simulation activity
Spin Filtering method (interaction of antiprotons non polarized with polarized hydrogen) 1. Test with protona at COSY + study of depolarisation from electrons
2. Measurements with antiprotons at AD/CERN (>2013)
The accelerator vacuum is going to be The accelerator vacuum is going to be Improved ! Improved !
The accelerator vacuum is going to be The accelerator vacuum is going to be Improved ! Improved !
INFN - JLab12 collaborationINFN - JLab12 collaboration
CEBAF: Continuous eCEBAF: Continuous e- -
beambeam• EnergyEnergymaxmax 6 GeV till may 6 GeV till may
20122012• EnergyEnergymaxmax 12 GeV : may 12 GeV : may 20132013 • 200 A, 75-85% polarization• Beam simultaneously delivered to 3 Halls
CEBAF @ Jefferson Lab (VA-USA)
A B CA B
Bari, Catania, Ferrara, Bari, Catania, Ferrara, Genova, ISS, LNF, RMI, Genova, ISS, LNF, RMI,
RMIIRMII
Reseachers+ engineers : 47 (32.5
FTE)
Technical staff: 31 (12.7 FTE)20102010: 41/29.5 FTE20112011: 47/32.5 FTE
• INFN @ JLab since 1991• In 2009 all INFN groups
merged into the JLAB12 JLAB12 collaboration collaboration
Hall A: Hall A: 2 high resolution 2 high resolution spectrometersspectrometers
Hall B:Hall B: Large angle spectrometerLarge angle spectrometer
INFN roles at JLABINFN roles at JLAB
• D. Bettoni, Member of the JLab Program Advisory Committee, 2010-today
• M. Ripani, CLAS Collaboration Chair, 2009-today
• R. De Vita, Secretary of the CLAS Speakers Committee, 2006-today
• M. Battaglieri, Chair of the CLAS Speakers Committee, 2005-today
• P. Rossi, Chair of the CLAS Service Work Committee, 2004-today
• P. Rossi, Member of the JLab Program Advisory Committee, 2010
• M. Ripani, Member of the JLab Program Advisory Committee, 2006-2009
• R. De Vita, Member of the JLab User Group Board of Directors, 2005-2007
• R. De Vita, Member of the CLAS Speakers Committee, 2003-2006
• N. Bianchi, Member of the JLab Program Advisory Committee, 2003-2005
• M. Battaglieri, Member of the CLAS Speakers Committee, 2001-2005
• P. Rossi, Member of the CLAS Service Work Committee, 2003-2004
• M. Taiuti, Chair of the CLAS Structure of the Nucleon Working Group, 2001-2004
• M. Taiuti, Member of the JLab Program Advisory Committee, 2000-2002
• E. De Sanctis, Member of the JLab Program Advisory Committee, 1997-1999
• G. Ricco, Member of the JLab Program Advisory Committee, 1995-1996
Italian Collaborators have been covering relevant roles in the Jefferson Lab community, as member of committees and chair of working groups and collaborations:
High Resolution Spectrometer
(HRS) Pair, andlarge installation
experiments
High Resolution Spectrometer
(HRS) Pair, andlarge installation
experiments
A
BBCLAS
upgraded to higher (1035)
luminosity and coverage
CLAS upgraded to higher (1035)
luminosity and coverage
Nucleon structure via Nucleon structure via generalized parton generalized parton
distributionsdistributions..
Nucleon structure via Nucleon structure via generalized parton generalized parton
distributionsdistributions..
SRC, FFs, Hypernuclear, SRC, FFs, Hypernuclear, Standard Model studies Standard Model studies
(PV, Moller)(PV, Moller)
SRC, FFs, Hypernuclear, SRC, FFs, Hypernuclear, Standard Model studies Standard Model studies
(PV, Moller)(PV, Moller)
RICH (Hall B)RICH (Hall B)
Central Neutron Detector (Hall B)Central Neutron Detector (Hall B)
Forward tagger (Hall B)Forward tagger (Hall B)
RICH (Hall B)RICH (Hall B)
Central Neutron Detector (Hall B)Central Neutron Detector (Hall B)
Forward tagger (Hall B)Forward tagger (Hall B)
Super Bite Spectrometer-tracking (Hall A)Super Bite Spectrometer-tracking (Hall A)
RICH (Hall A)RICH (Hall A)
Super Bite Spectrometer-tracking (Hall A)Super Bite Spectrometer-tracking (Hall A)
RICH (Hall A)RICH (Hall A)
INFN contribution INFN contribution to the upgrades and new detectors for 12 GeV program to the upgrades and new detectors for 12 GeV program
INFN contribution for 12 GeV programINFN contribution for 12 GeV programGEM tracker for hall A GEM tracker for hall A
DESY beam test in Dec/09: setupDESY beam test in Dec/09: setup
Silicon Tracker+ scintillator fingers
2x 10x10 cm2 GEM prototypes
HV Power Supply
Beam
overlap with the Olympus developmentoverlap with the Olympus development
A Forward tagger for CLAS12A Forward tagger for CLAS12
The geometry of the Forward Tagger Calorimeter based on the PbW04 crystals has been implemented in the CLAS12 GEANT4 MC
Massive simulations of the e.m. background to determine - Rates - Radiation dose - Optimize Moeller shield in progress
Tests with cosmic rays and radioactive sources in Genova Tests with 500 MeV electrons at the BTF in Frascati
Tests with cosmic rays and radioactive sources in Genova Tests with 500 MeV electrons at the BTF in Frascati
GeV/c 1 2 3 4 5 6 7 8 9 10
/K
/p
K/p
RIC
HRIC
H
TOF
TOF
LTCCHTCC
HTCC
LTCC
TOF
LTCCLTCC
A RICH detector for CLAS12
20
Ongoing R&D activities:Ongoing R&D activities:
Improve simulation Improve simulation Geant 4 (Argonne, ….) + GEMC (JLab…) Geant 4 (Argonne, ….) + GEMC (JLab…)
Reduce costs Reduce costs mirrors and light concentrators mirrors and light concentrators
Validate simulations and check performancesValidate simulations and check performances Test components (Glasgow, ….)Test components (Glasgow, ….) Prototype (INFN groups, JRA-WP3) Prototype (INFN groups, JRA-WP3)
Ongoing R&D activities:Ongoing R&D activities:
Improve simulation Improve simulation Geant 4 (Argonne, ….) + GEMC (JLab…) Geant 4 (Argonne, ….) + GEMC (JLab…)
Reduce costs Reduce costs mirrors and light concentrators mirrors and light concentrators
Validate simulations and check performancesValidate simulations and check performances Test components (Glasgow, ….)Test components (Glasgow, ….) Prototype (INFN groups, JRA-WP3) Prototype (INFN groups, JRA-WP3)
pp collision at 7 TeV
Nuclear Structure and reaction mechanisms Nuclear Structure and reaction mechanisms
5-10 MeV/u5-10 MeV/u 50 MeV/u 50 MeV/u Heavy-ionsHeavy-ions
GAMMA- PRISMA- EXOTIC- NUCLEX
MAGNEX- LNS_Stream - Fribs - Exochim
Reactions and decays Reactions and decays
• Nuclear structure •Equation of state
astrophysical astrophysical implications implications nucleosynthesisnucleosynthesis
Exctreme conditions Exctreme conditions for nuclei for nuclei
+ coll with GSI and + coll with GSI and GANILGANIL
AGATA Demonstrator inauguration 9/5/2010
AGATA Demonstrator inauguration 9/5/2010
70Ni 72Ni
Several Several data analysisdata analysisin progressin progress
effect of neutron orbitalsand role of tensor tensor forceforce
effect of neutron orbitalsand role of tensor tensor forceforce
GANIL LNLLNL
Measurement campaign (with ALPI)Measurement campaign (with ALPI)
Focussed on nuclear collectivity in nuclei Focussed on nuclear collectivity in nuclei From low-lying vibrations and rotations to giant resonances
Excellent energy resolution and high count rates
Excellent energy resolution and high count rates
16 keV
16C
13B
10Be
7Li
Fragmentation of beams at LNS : Fragmentation of beams at LNS : reaction with reaction with 1616CC and and 1313BeBe at 50 MeV/u at 50 MeV/u
ActivityActivityExp. FRAG and Exp. FRAG and EXOCHIMEXOCHIM
Prelim
inar
y
Prelim
inar
y
Elastic cross-section Elastic cross-section
1616CC 1616CC
1313BeBe 1313BeBe
1010BeBe
MeasurementsMeasurementswith with CHIMERACHIMERA10104-54-5 pps pps
Unique energy interval ! Unique energy interval !
Trasmission will be improved Production studies in progress
18O primary beam -magnet setting on 11Be
strip 140 mm thick
18O primary beam -magnet setting on 11Be
strip 140 mm thick
Nuclear astrophysics and interdisciplinary Nuclear astrophysics and interdisciplinary reserachreserach
Gamow peak
tunneling throughCoulomb barrier exp -(E0/E)1/2
Maxwell-Boltzmanndistribution
E1/2exp(-E/kT)
rela
tive p
rob
ab
ilit
yenergykT E0
Reactions at stellar Reactions at stellar energies for : energies for :
•Energy generationEnergy generation• NucleosynthesisNucleosynthesis (exp LUNA, ASFIN e (exp LUNA, ASFIN e ERNA) ERNA) Energie ≈ MeV
•Annichilation of anti protons in nuclei 5keV – 5 MeVregion of cosmological interest ASACUSA + R&D AEGISASACUSA + R&D AEGIS
• Pauli principle violation in atomic transitions (LNGS) (exp (exp VIP)VIP)
•Neutron capture for Neutron capture for astrophysics and astrophysics and application in reactors of application in reactors of new generation. new generation.
n_TOF al CERNn_TOF al CERN
Cyclotron 750 μA, 70 MeV (max) for protons in two exit ports: •RIB - up to 300 μA p on UCx•Application - up to 500 μA
Cyclotron 750 μA, 70 MeV (max) for protons in two exit ports: •RIB - up to 300 μA p on UCx•Application - up to 500 μA
Additional target station (special plants second priority)RIB or neutron production
Additional target station (special plants second priority)RIB or neutron production
UCx target station 1013 fission/s
UCx target station 1013 fission/s
High Resolution Mass Spectrometer 1/20000
High Resolution Mass Spectrometer 1/20000
Charge Breeder1+ n+Charge Breeder1+ n+
transport/beam cooler/separator
(Post Accelerator)
SPES ISOL facility SPES ISOL facility SPES ISOL facility SPES ISOL facility
G.PreteALPI layout
•ALICE is collecting data and producing papers. Computing and Upgrade?
• The first experimental campaign with the AGATA demonstrator has started at LNL. The realization of ¼ of solid angle is in progress. Nuclei at extremes are being investigated.
•Esperiments engaged in upgrades such as JLAB and LUNA are progressing.
• Several relevant results are obtained with the analysis of experiments under way. They are important to guide the future programs.
We count on the activity at JLAB We count on the activity at JLAB for which also in the future (as in the for which also in the future (as in the past) we expect outstanding results !past) we expect outstanding results !
CONCLUSION CONCLUSION
Equipments / Experiments Matrix @ 12 GeVHD
TargetCentral
DetectorRICH
CLAS12ForwardTagger
GEMTracker
SiDetector
BA X X
CT X
FE X
GE X X X X
ISS X X X
LNF X X X
RM1 X X X
RM2 X X X
Physics TMD GPD TMD MesonFF, TMD,
PVESFF, TMD
33