roberto francisco pérez benito on behalf the hermes collaboration european graduate school lecture...
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![Page 1: Roberto Francisco Pérez Benito On behalf the HERMES Collaboration European Graduate School Lecture Week on Hadron Physics Jyväskylä, Aug 25-29, 2008 HERMES](https://reader030.vdocuments.us/reader030/viewer/2022032704/56649d825503460f94a66f7a/html5/thumbnails/1.jpg)
Roberto Francisco Pérez BenitoOn behalf the HERMES Collaboration
European Graduate School
Lecture Week on Hadron PhysicsJyväskylä, Aug 25-29, 2008
HERMES Recoil Detector
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OutlineOutlineOutlineOutline
Motivation
The Hermes Recoil Detector
Performance
Outlook
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The Spin Structure of the NulceonThe Spin Structure of the NulceonThe Spin Structure of the NulceonThe Spin Structure of the NulceonNulceon Spin:
Spin of quarks
measured in DIS
HERMES: Spin of gluons, first Measurements
expected to be small Orbital angular momentum of
quarks Orbital angular momentum of
gluons
unknown
Accss to via Deeply Virtual Compton Scattering (DVCS)
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Generalized Parton Distributions (GPDs)Generalized Parton Distributions (GPDs)Generalized Parton Distributions (GPDs)Generalized Parton Distributions (GPDs)
Ji Sum Rule – Ji, PRL 78(1997)610
parton longitudinal momentum fractions
fraction of the momentum transfer
invariant momentum transfer to the nucleon
GPDs
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GPDs and the DVCS processGPDs and the DVCS processGPDs and the DVCS processGPDs and the DVCS process
DVCS final state is indistinguishable from theBethe-Heitler Process (BH) → Amplitudes add Coherently
Photon-Production cross section:
Interference Term
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DVCS MeasurementsDVCS MeasurementsDVCS MeasurementsDVCS Measurements
calculable in QED with the knowledge of the Form Factors
is parameterized in terms of Compton Form Factors
(convolutions of GPDs )
At HERMES kinematics:
GPDs accessible through cross-section differences and azimuthal asymmetries via interference term I → Magnitude + Phase(GPDs enter in linear combinations)
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The HERMES Spectrometer (before 2006)The HERMES Spectrometer (before 2006)The HERMES Spectrometer (before 2006)The HERMES Spectrometer (before 2006)
Polarize gas targets: H,D,HeUnpolarize gas targets: H,D,N,He,Ne,Xe,Kr
Fixed target experiment (uses 27.6 GeV/c HERA lepton Beam)
Recoiling proton undetected large background contamination (15%)
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Exclusivity for DVCS via Missing Mass Exclusivity for DVCS via Missing Mass Exclusivity for DVCS via Missing Mass Exclusivity for DVCS via Missing Mass Exactly one DIS lepton and one photon detected in the Calorimeter.
Recoiling proton undetected.
Exclusivity via Missing Mass
exclusive region
Overall background contribution in exclusive region
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The HERMES Spectrometer (2006 - 2007)The HERMES Spectrometer (2006 - 2007)The HERMES Spectrometer (2006 - 2007)The HERMES Spectrometer (2006 - 2007)
Recoil detector installed for the last two years of data taking Recoiling proton detected background contamination <1%
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Recoil DetectorRecoil Detector Recoil DetectorRecoil Detector Photon Detector 3 layers of Tungsten/Scintillator
1 Tesla Superconducting Solenoid
Scintillating Fiber Detector 2 Barrels 2 Parallel & 2 Stereo-Layers in
each barrelSilicon Detector
2 Layer of 16 double-sides sensors 97×97 mm2 active area each Inside HERA vacuum
Target Cell
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Alignment of the SFT Alignment of the SFT Alignment of the SFT Alignment of the SFT
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Measurements of dedicated SFT run were used and tested on cosmic data collected with Recoil detector
Residuals (280 µm) are in good agreement with expectations from ideally aligned Monte-Carlo (220 µm)
SFT Paralleltop
=0.28mm
Si and PD alignment respect SFT
Results of Alignment of SFT Results of Alignment of SFT Results of Alignment of SFT Results of Alignment of SFT
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Ep Elastic ScatteringEp Elastic ScatteringEp Elastic ScatteringEp Elastic Scattering
Detect scattered electron in the Forward spectrometer and protons in the Recoil
Correlation of angles reconstructed in the Forward spectrometer and the Recoil Detector can be used for the relative alignment of these detector systems
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Momentum ReconstructionMomentum Reconstruction Momentum ReconstructionMomentum Reconstruction
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Momentum ReconstructionMomentum Reconstruction Momentum ReconstructionMomentum Reconstruction
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Momentum ReconstructionMomentum Reconstruction Momentum ReconstructionMomentum Reconstruction
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HERMES magnet
Recoil detector Energy loss of single fiber from pions Leading fibers from tracks were selected MIP’s position are stable from different time periods
Energy Deposit of MIP‘s Energy Deposit of MIP‘s Energy Deposit of MIP‘s Energy Deposit of MIP‘s
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Recoil Particle IdentificationRecoil Particle IdentificationRecoil Particle IdentificationRecoil Particle Identification
HERMES magnet
Recoil detector
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Collected statistic (preliminary) with recoil detector
Electron beam 2006 (only SFT operational):
H : 5k DVCS (3Mio. DIS), D : 1k DVCS (0.8Mio. DIS)
Positron beam 2006/07 (all subdetectors fully operational)
H : 41k DVCS (38Mio. DIS), D : 7.5k DVCS (10Mio. DIS)
Data tacking and PerformanceData tacking and PerformanceData tacking and PerformanceData tacking and Performance
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Outlook Outlook Outlook Outlook Analysis of data with Recoil Detector
for exclusive photons and mesons Exclusive meson cross-sections Exclusive meson cross-section ratios Spin Density Matrix Elements Exclusive πˉ and π° impossible without Recoil Detector!