hadronic multi-particle final state measurements with clas at jefferson lab
DESCRIPTION
Hadronic Multi-particle Final State Measurements with CLAS at Jefferson Lab. Laird Kramer Florida International University Neutrino Scattering, March 2003. Outline. Overview of CLAS Physics Program Description of CLAS Samples of CLAS data and analysis Future nuclear target experiments - PowerPoint PPT PresentationTRANSCRIPT
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Hadronic Multi-particle Final Hadronic Multi-particle Final State Measurements with CLAS State Measurements with CLAS
at Jefferson Labat Jefferson Lab
Laird KramerLaird Kramer
Florida International UniversityFlorida International University
Neutrino Scattering, March 2003Neutrino Scattering, March 2003
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OutlineOutline
Overview of CLAS Physics ProgramOverview of CLAS Physics Program
Description of CLASDescription of CLAS
Samples of CLAS data and analysisSamples of CLAS data and analysis
Future nuclear target experimentsFuture nuclear target experiments
ConclusionsConclusions
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CLAS: the CLAS: the CCEBAF EBAF LLarge arge AAcceptance cceptance SSpectrometer in Hall B at JLABpectrometer in Hall B at JLAB
International collaboration of 160 scientistsInternational collaboration of 160 scientists
Physics data taking began end of 1997Physics data taking began end of 1997
17 major production runs completed17 major production runs completed
Wide variety of run conditions: Wide variety of run conditions: Electron/photon beams, 0.5<E<6 GeV (polarized)Electron/photon beams, 0.5<E<6 GeV (polarized)
Targets: Targets: 1,21,2H (including polarized), H (including polarized), 3,43,4He, He, 1212C, C, 5656Fe, etc.Fe, etc.
50 PhD theses underway or completed50 PhD theses underway or completed
More info at http://www.jlab.org/Hall-BMore info at http://www.jlab.org/Hall-B
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CLAS Physics HighlightsCLAS Physics HighlightsBroad program: over 50 experimentsBroad program: over 50 experiments
Physics of excited nucleons (N* program)Physics of excited nucleons (N* program)Neutron electromagnetic form factorNeutron electromagnetic form factorPolarized structure functionsPolarized structure functionsDeep virtual Compton scattering (GPD’s)Deep virtual Compton scattering (GPD’s)Quark/hadron propagation through nucleiQuark/hadron propagation through nucleiSemi-inclusive deep inelastic scatteringSemi-inclusive deep inelastic scatteringExotic meson searchesExotic meson searchesElementary hyperon photoproductionElementary hyperon photoproductionTwo-nucleon correlations in light nucleiTwo-nucleon correlations in light nuclei
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Charged particle angles 8° - 144°
Neutral particle angles 8° - 70°
Momentum resolution ~0.5% (charged)
Angular resolution ~0.5 mr (charged)
Identification of p, +/-, K+/K-, e-/e+
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Typical Run ConditionsTypical Run Conditions
Luminosity of 1034 cm-2s-1 (LH2 target)
106 hadronic interactions/second
Up to 4000 Hz event rate
Trigger: single electron
Data transfer rate: up to 20 MByte/s (~ 1 TByte/day)
Acquire 10 – 30 billion triggers/year
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Physics of Excited NucleonsPhysics of Excited NucleonsN* programN* program
Resonance transition form factorsResonance transition form factors N-N- transition transition
Second resonance region (e.g. SSecond resonance region (e.g. S11))
N-N- axial form factor axial form factor
Quark model ‘missing resonances’Quark model ‘missing resonances’ Can find them in unexplored decay channels?Can find them in unexplored decay channels?
Models have correct degrees of freedom?Models have correct degrees of freedom?
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Inclusive scattering in the resonance region
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Q2 (G
eV2 )
W (GeV)
N(940)(1232)
N(1520)
N(1680)
CLAS: ep eX, E = 4 GeV
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o
CLAS: ep epX, E = 4 GeVW
(GeV
)
Missing Mass (GeV)
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ep
eX
, E =
4 G
eV
Inclusive
2 hadrons2 hadrons
2 hadrons
3 hadrons
4 hadrons
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cos(*
)
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N-
N-
tran
sitio
n tr
ansi
tion
ampl
itude
sam
plitu
des
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Quark/Hadron Propagation Quark/Hadron Propagation through Nucleithrough Nuclei
Space-time properties of hadronizationSpace-time properties of hadronizationMass, size, pMass, size, pT, , , z, Q, z, Q2, and flavor dependences of , and flavor dependences of hadron formation lengthshadron formation lengthsGluon emissionGluon emission
Transverse momentum broadeningTransverse momentum broadeningQuark-gluon correlationsQuark-gluon correlationsQuark energy lossQuark energy loss
6 GeV experiment coming in June 20036 GeV experiment coming in June 2003New collaborators welcomeNew collaborators welcome
11 GeV experiment (in 2010-2012?)11 GeV experiment (in 2010-2012?)
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Space-time Picture of HadronizationSpace-time Picture of Hadronization
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Nuclear Quark/Hadron Propagation Nuclear Quark/Hadron Propagation Experimental MethodExperimental Method
Use a range of targets, light to heavyUse a range of targets, light to heavy1H, H, 2H, H, 14N, N, 56Fe, Fe, 84Kr, Kr, 197AuAu
DIS kinematics + measure hadronsDIS kinematics + measure hadrons
Single electron triggerSingle electron trigger
Nuclear medium modifies fragmentation Nuclear medium modifies fragmentation functions and pfunctions and pT distributionsdistributions
6 GeV beam: Q6 GeV beam: Q2 ≤ 4 GeV ≤ 4 GeV2, , ≤ 5 GeV ≤ 5 GeV
12 GeV beam: Q12 GeV beam: Q2 ≤ 9 GeV ≤ 9 GeV2, , ≤ 9 GeV ≤ 9 GeV
Measure Measure , , ’, ’, p,p,
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Recent Data from HERMES at HERARecent Data from HERMES at HERA
Data: Eur. Phys. J. C20 (2001) 479.Theory: nucl-th/9607036 for gluon bremsstrahlung model,
Phys. Rev. Lett. 89 (2002) for twist-4 pQCD model.
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Anticipated CLAS Data at 6 GeVAnticipated CLAS Data at 6 GeV
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Kin
emat
ic C
over
age,
12
GeV
Kin
emat
ic C
over
age,
12
GeV
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Neutral particle Neutral particle detection for detection for fragmentation fragmentation events at 11 GeV events at 11 GeV (LEPTO simulation, (LEPTO simulation, no vertex cut)no vertex cut)
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Some PotentiallySome PotentiallyInterested CollaboratorsInterested Collaborators
Will Brooks, JlabWill Brooks, JlabMaurik Holtrop, UNHMaurik Holtrop, UNHDavid Ireland, GlasgowDavid Ireland, GlasgowMauro Taiuti, INFN Mauro Taiuti, INFN Larry Weinstein, ODULarry Weinstein, ODUSteve Wood, JlabSteve Wood, JlabLaird Kramer, FIU Laird Kramer, FIU … …
Arie Bodek, RochesterArie Bodek, RochesterJorge Morfin, FNALJorge Morfin, FNALIngo Schienbein, DESYIngo Schienbein, DESYJan Sobczyk, U. Jan Sobczyk, U. WroclawWroclawMakoto Sakuda, KEKMakoto Sakuda, KEKEmmanuel Paschos, U. Emmanuel Paschos, U. DortmundDortmundShri Singh, Aligargh Shri Singh, Aligargh Moslem U.Moslem U.
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ConclusionConclusion
CLAS has taken a huge volume of new CLAS has taken a huge volume of new data including multi-hadron final statesdata including multi-hadron final states
N* and nuclear data likely to be of interest N* and nuclear data likely to be of interest to neutrino communityto neutrino community
Collaborative connection likely to be most Collaborative connection likely to be most fruitful – many potential opportunities for fruitful – many potential opportunities for collaborationcollaboration
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Hadrons accessible for formation length studiesHadrons accessible for formation length studiesC
LAS
at 1
1 G
eV