MENU 2013 –Rome, 2/10/2013
The Forward Tagger facility for low Q2 experiments at Jefferson Laboratory
- A. Celentano
The Forward Tagger facility for low Q 2 experiments at Jefferson - - PowerPoint PPT Presentation
The Forward Tagger facility for low Q 2 experiments at Jefferson Laboratory A. Celentano INFN-Genova MENU 2013 Rome, 2/10/2013 Outline The low Q 2 electron scattering experimental technique: kinematics, polarization, and physical
MENU 2013 –Rome, 2/10/2013
MENU 2013 –Rome, 2/10/2013
kinematics, polarization, and physical motivations
MENU 2013 –Rome, 2/10/2013
Photo-production program with quasi-real photons: low Q2 electron scattering
CLAS12 detector
new Forward Tagger facility
Forward Tagger
Main physical motivation: Spectroscopy
MENU 2013 –Rome, 2/10/2013
Meson spectroscopy: standard PWA on H target and spectroscopy on He4 and other gas targets
suppress backgrounds
Need spin-fip for exotic quantum numbers No spin-fip for exotic quantum number
MENU 2013 –Rome, 2/10/2013
Kinematic variables: Virtual photon polarization, defined event by event: Q2 vs Eγ εΤ vs Eγ
Transverse linear polarization Longitudinal polarization
MENU 2013 –Rome, 2/10/2013 V.M. Budnev, et al., Physics Reports, Volume 15, Issue 4, 1975
Low Q2 electron scattering is competitive and complementary to real photo-production. Equivalent photon-flux approximation: In the Forward Tagger kinematic range:
✔ Luminosity:1035 cm-2 s-1 ✔ σΤΟΤ
γ ∼ 100 µbarn
Expected event rate: 7 kHz Equivalent photon flux:
✔ On a 40 cm long LH2 target
MENU 2013 –Rome, 2/10/2013
<Q2> ~ 5 10-5 GeV2 HERA e- / p collider
<Q2> ~ 10-1 GeV2 160 GeV/c µ- beam on 6LiD target
1 missing e− at ~ 0 deg selected
Mass spectra show evidence of low cross-section mesons expected in these photo-production channel.
MENU 2013 –Rome, 2/10/2013
Beam is delivered simultaneously to the 3 experimental halls.
MENU 2013 –Rome, 2/10/2013
MENU 2013 –Rome, 2/10/2013
Forward Detector (5°< θ < 35°):
(HTCC)
(LTCC)
Central Detector (θ > 35°) :
Micromegas tracker (SVT)
High acceptance (~4π) detector, designed to work @ luminosity 1035 cm-2 s-1
MENU 2013 –Rome, 2/10/2013
Forward Tagger design characteristics
3 Components :
PbWO4 calorimeter: measure the energy of scattered electrons with few % resolution. Scintillation hodoscope: distinguish photons from electrons. Micromegas tracker: determine the electron scattering plane.
MENU 2013 –Rome, 2/10/2013
MENU 2013 –Rome, 2/10/2013
FT-Cal rad dose @ nominal CLAS12 luminosity Rad/h
in CLAS12
CLAS12 Signal and background rates @ CLAS12 nominal luminosity 1035 cm-2 s-1
MENU 2013 –Rome, 2/10/2013
including threshold and reconstruction effects
Recoil electron Virtual photon Virtual photon energy resolution increment due to 1/E factor, E=11 GeV
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Foreseen energy resolution
Design:
Forward Tagger Facility “core” component. Requirements:
MENU 2013 –Rome, 2/10/2013
FT-Cal crystals properties measured with ACCOS facility @ CERN
MENU 2013 –Rome, 2/10/2013
G=1
FT-Cal APDs characterized with a custom- designed facility, in the temperature range 0° – 25°
Gain measured with “DC-technique”: measure I vs Vb under constant illumination, subtract dark current, and re-normalize to G=1 (Vb < 50 V)
MENU 2013 –Rome, 2/10/2013
Readout board: JLab-made FADC
FEE electronics: custom amplifier circuit
APD capacitance
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Design:
elements each, 30x30 and 15x15 mm2
coupled to Hamamatsu 3x3 mm2 SiPMs
coincidence with FT-Cal Detector design supported by dedicated GEANT4 simulations of its optical response
20 detected photons expected for MIP
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Custom electronics developed for FT-Hodo SiPM readout
boards
MENU 2013 –Rome, 2/10/2013
Amplitude Charge
Results obtained with a laser test-bench setup:
intensity and frequency
✔ Single phe peaks well resolved and
separated from background
✔ SiPM gain tunable within factor ~10 wrt
nominal working point
Nominal gain
dG / G ~ 10
MENU 2013 –Rome, 2/10/2013
Amplitude Charge
Results obtained with a laser test-bench setup:
intensity and frequency
✔ Single phe peaks well resolved and
separated from background
✔ SiPM gain tunable within factor ~10 wrt
nominal working point
Nominal gain
dG / G ~ 10
MENU 2013 –Rome, 2/10/2013
Design:
with 500 μm strip readout
DREAM ASIC
tracker
MENU 2013 –Rome, 2/10/2013
16 channel FT-Cal prototype:
between few MeV (cosmic rays) to 4 GeV (e- beam test)
the energy resolution temperature dependence
conditions
Design:
15x15x200 mm3
HV distribution
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First FT-proto tests performed with cosmic- rays setup
counters
Cosmic rays 500 MeV e- beam
The measure was aimed to:
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DAΦNE LINAC BTF
The BTF test beam is obtained attenuating the primary LINAC electron beam delivered to the DAFNE machine.
1 - 105 e-/bunch
BTF beam properties:
MENU 2013 –Rome, 2/10/2013
DAΦNE LINAC BTF
The BTF test beam is obtained attenuating the primary LINAC electron beam delivered to the DAFNE machine.
1 - 105 e-/bunch
BTF beam properties:
DETECTOR BEAM
MENU 2013 –Rome, 2/10/2013
FT-CAL BTF test results
agreement
the experimental energy resolution with MC results for Ee>1.5 GeV
noise contribution Measure @0°C
MENU 2013 –Rome, 2/10/2013
photons: competitive and complementary to “real” photo-production experiments.
perform quasi-real photo-production experiments. Main physical motivation: spectroscopy
confirmed the detector operational principles, provided a first measure of the foreseen performances, and was used to tune MC parameters.
MENU 2013 –Rome, 2/10/2013
MENU 2013 –Rome, 2/10/2013
Neglect q-dependent terms due to EM current conservation:
Resulting amplitude is the product of two terms:
Reaction amplitude in the OPE approximation: Completeness relation for virtual-photon polarization:
MENU 2013 –Rome, 2/10/2013
MENU 2013 –Rome, 2/10/2013