The Forward Tagger facility for low Q 2 experiments at Jefferson - - PowerPoint PPT Presentation

the forward tagger facility for low q 2 experiments at
SMART_READER_LITE
LIVE PREVIEW

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


slide-1
SLIDE 1

MENU 2013 –Rome, 2/10/2013

The Forward Tagger facility for low Q2 experiments at Jefferson Laboratory

  • A. Celentano

INFN-Genova

slide-2
SLIDE 2

MENU 2013 –Rome, 2/10/2013

Outline

  • The low Q2 electron scattering experimental technique:

kinematics, polarization, and physical motivations

  • The Forward Tagger Facility in Hall B at Jefferson Laboratory
  • Design overview
  • Foreseen performances
  • Rates and backgrounds
  • The Forward Tagger components: design and tests
  • FT-Cal
  • FT-Hodo
  • FT-Trck
  • The FT-Cal prototype
slide-3
SLIDE 3

MENU 2013 –Rome, 2/10/2013

Photo-production program with quasi-real photons: low Q2 electron scattering

  • Final state hadrons measured with the

CLAS12 detector

  • Low-angle scattered electron measured with the

new Forward Tagger facility

Forward Tagger

Low Q2 experiments with CLAS12

Main physical motivation: Spectroscopy

slide-4
SLIDE 4

MENU 2013 –Rome, 2/10/2013

Low Q2 experiments with CLAS12

Meson spectroscopy: standard PWA on H target and spectroscopy on He4 and other gas targets

  • Photoproduction: exotic quantum numbers are more likely produced by S=1 probe
  • Linear polarization: acts like a filter to disentangle the production mechanisms and

suppress backgrounds

  • Production rate: for exotics is expected to be comparable as for regular mesons

Need spin-fip for exotic quantum numbers No spin-fip for exotic quantum number

slide-5
SLIDE 5

MENU 2013 –Rome, 2/10/2013

Low Q2 electron scattering: kinematics

Kinematic variables: Virtual photon polarization, defined event by event: Q2 vs Eγ εΤ vs Eγ

Transverse linear polarization Longitudinal polarization

slide-6
SLIDE 6

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

Low Q2 electron scattering: equivalent photon flux

slide-7
SLIDE 7

MENU 2013 –Rome, 2/10/2013

Low Q2 electron scattering: examples

  • ZEUS:

<Q2> ~ 5 10-5 GeV2 HERA e- / p collider

  • COMPASS:

<Q2> ~ 10-1 GeV2 160 GeV/c µ- beam on 6LiD target

  • CLAS:
  • 6 GeV / c electron beam on proton target
  • Events with 1 proton, 4 γ,

1 missing e− at ~ 0 deg selected

  • 4 γ invariant mass measured

Mass spectra show evidence of low cross-section mesons expected in these photo-production channel.

slide-8
SLIDE 8

MENU 2013 –Rome, 2/10/2013

Continuous Electron Beam Accelerator Facility

  • E = 0.75 – 6 GeV
  • Imax = 100 µA - Hall A, C
  • Imax = 800 nA – Hall B
  • Duty Cycle ~ 100%
  • σ(E)/E ~ 2.5 x 10-5
  • Polarization ~ 80%

Beam is delivered simultaneously to the 3 experimental halls.

JLab @ 6 GeV

slide-9
SLIDE 9

MENU 2013 –Rome, 2/10/2013

JLab @ 12 GeV

slide-10
SLIDE 10

MENU 2013 –Rome, 2/10/2013

The CLAS12 detector in Hall B

Forward Detector (5°< θ < 35°):

  • Toroidal magnet (TORUS)
  • High threshold Cherenkov counter

(HTCC)

  • Drift chammbers (Region 1, 2, 3)
  • Low threshold Cherenkov counter

(LTCC)

  • TOF counters (FTOF)
  • EM calorimeter (EC)

Central Detector (θ > 35°) :

  • Solenoidal field (SOLENOID)
  • Silicon vertex tracker +

Micromegas tracker (SVT)

  • TOF counters (CTOF)
  • Neutron detector (CND)

High acceptance (~4π) detector, designed to work @ luminosity 1035 cm-2 s-1

slide-11
SLIDE 11

MENU 2013 –Rome, 2/10/2013

The Forward Tagger Facility

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.

slide-12
SLIDE 12

MENU 2013 –Rome, 2/10/2013

The Forward Tagger Facility

slide-13
SLIDE 13

MENU 2013 –Rome, 2/10/2013

FT rates and backgrounds

FT-Cal rad dose @ nominal CLAS12 luminosity Rad/h

  • Signal rate ~ 1 kHz
  • 1 e- detected in FT in coincidence with an hadronic event

in CLAS12

  • Total background rate ~ 100 MHz
  • Low energy (< MeV) particles, e- and γ
  • In the FT energy range (0.5 – 4.5 GeV) ~180 kHz
  • Highly suppressed by tight time coincidence with

CLAS12 Signal and background rates @ CLAS12 nominal luminosity 1035 cm-2 s-1

slide-14
SLIDE 14

MENU 2013 –Rome, 2/10/2013

FT foreseen (MC) performances

  • FT energy resolution has been evaluated trough detailed MC simulations,

including threshold and reconstruction effects

  • Crystals shape and dimensions optimized to maximize the energy resolution

Recoil electron Virtual photon Virtual photon energy resolution increment due to 1/E factor, E=11 GeV

slide-15
SLIDE 15

MENU 2013 –Rome, 2/10/2013

The FT-Cal

Foreseen energy resolution

Design:

  • 332 channels
  • PbWO4 crystals, 15x15x200 mm3
  • Large Area APD readout (10x10 mm2)
  • Custom FEE
  • 0° operating temperature

Forward Tagger Facility “core” component. Requirements:

  • Strong radiation hardness
  • Good Energy and Timing resolution
  • Small radiation length and Moliere Radius
  • Compatible with high magnetic field
slide-16
SLIDE 16

MENU 2013 –Rome, 2/10/2013

FT-Cal crystals

FT-Cal crystals properties measured with ACCOS facility @ CERN

  • Dimensions
  • Light yield
  • Optical transmission
  • Radiation hardness
slide-17
SLIDE 17

MENU 2013 –Rome, 2/10/2013

FT-Cal APDs

G=1

FT-Cal APDs characterized with a custom- designed facility, in the temperature range 0° – 25°

  • Gain vs Vb and T
  • Dark current vs Vb and T
  • Stability

Gain measured with “DC-technique”: measure I vs Vb under constant illumination, subtract dark current, and re-normalize to G=1 (Vb < 50 V)

slide-18
SLIDE 18

MENU 2013 –Rome, 2/10/2013

FT-Cal FEE and REO

Readout board: JLab-made FADC

  • Employed for CLAS12 fast detectors
  • 250 Msamples/s
  • 12 bit resolution
  • 2 Volts maximum input signal
  • 16 channels
  • VXS extension
  • Online signal elaboration trough on-board FPGA
  • Energy
  • Timing
  • Evolute trigger capabilities

FEE electronics: custom amplifier circuit

  • Gain ~ 1800
  • Noise RMS ~ 5 mV (ENE ~ 5 MeV)
  • Input impedance matched to

APD capacitance

  • Bandwidth ~ 20 MHz
slide-19
SLIDE 19

MENU 2013 –Rome, 2/10/2013

The FT-Hodo

Design:

  • Plastic Scintillator tiles: 2 layers with 116

elements each, 30x30 and 15x15 mm2

  • Readout based on WLS fibers

coupled to Hamamatsu 3x3 mm2 SiPMs

  • Custom FEE with single-channel tunable gain
  • 1 ns foreseen timing resolution for precise

coincidence with FT-Cal Detector design supported by dedicated GEANT4 simulations of its optical response

20 detected photons expected for MIP

slide-20
SLIDE 20

MENU 2013 –Rome, 2/10/2013

FT-Hodo FEE

Custom electronics developed for FT-Hodo SiPM readout

  • Modular design
  • 16 channels mezzanine cards connected to 2 8-channels amplifier

boards

  • Up to 15 mezzanines in the same system (240 channels)
  • 1 controller card
  • Custom crate, VME-9U mechanical compliant
  • Single channel amplifier: transimpedance configuration
  • 2 stage amplifier
  • Gain ~ 660
  • ENC ~ 0.5 phe
  • Common SiPM HV for groups of 8
  • Individual HV tunable within + 2 V for fine gain tuning
slide-21
SLIDE 21

MENU 2013 –Rome, 2/10/2013

Amplitude Charge

FT-Hodo FEE

Results obtained with a laser test-bench setup:

  • 200 ps width laser bunches, with variable

intensity and frequency

  • Signal acquired with digital oscilloscope
  • Trigger from the laser sync signal

✔ Single phe peaks well resolved and

separated from background

✔ SiPM gain tunable within factor ~10 wrt

nominal working point

Nominal gain

dG / G ~ 10

slide-22
SLIDE 22

MENU 2013 –Rome, 2/10/2013

Amplitude Charge

FT-Hodo FEE

Results obtained with a laser test-bench setup:

  • 200 ps width laser bunches, with variable

intensity and frequency

  • Signal acquired with digital oscilloscope
  • Trigger from the laser sync signal

✔ Single phe peaks well resolved and

separated from background

✔ SiPM gain tunable within factor ~10 wrt

nominal working point

Nominal gain

dG / G ~ 10

slide-23
SLIDE 23

MENU 2013 –Rome, 2/10/2013

The FT-Tracker

Design:

  • Two double layers of bi-face bulk Micromegas

with 500 μm strip readout

  • Custom FE electronics: 3392 channels, based on

DREAM ASIC

  • Same technology adopted for CLAS12 central

tracker

slide-24
SLIDE 24

MENU 2013 –Rome, 2/10/2013

FT-Cal prototype

16 channel FT-Cal prototype:

  • Measure energy resolution and linearity

between few MeV (cosmic rays) to 4 GeV (e- beam test)

  • Measure

the energy resolution temperature dependence

  • Measure the electronic noise in realistic

conditions

  • Validate MonteCarlo simulations

Design:

  • 4x4 matrix of PbWO4 matrix, each

15x15x200 mm3

  • Large Area APD readout (10x10mm2)
  • Copper shield for thermal stabilization
  • Custom motherboard for signal, LV,

HV distribution

slide-25
SLIDE 25

MENU 2013 –Rome, 2/10/2013

FT-Cal prototype test with cosmics ray

First FT-proto tests performed with cosmic- rays setup

  • Detector placed in between 3 plastic scintillators

counters

  • Scintillators hits positions provide cosmic track
  • Trigger given by the 3 counters coincidence
  • Cal. constants ratio

Cosmic rays 500 MeV e- beam

The measure was aimed to:

  • Demonstrate operational principles
  • Test the detector performances
  • Provided a first estimate of cal. Constants
  • Tune MC simulations
slide-26
SLIDE 26

MENU 2013 –Rome, 2/10/2013

FT-Cal prototype test @ LNF BTF

DAΦNE LINAC BTF

The BTF test beam is obtained attenuating the primary LINAC electron beam delivered to the DAFNE machine.

  • Variable intensity:

1 - 105 e-/bunch

  • Variable electron energy: 25 – 500 MeV

BTF beam properties:

slide-27
SLIDE 27

MENU 2013 –Rome, 2/10/2013

FT-Cal prototype test @ LNF BTF

DAΦNE LINAC BTF

The BTF test beam is obtained attenuating the primary LINAC electron beam delivered to the DAFNE machine.

  • Variable intensity:

1 - 105 e-/bunch

  • Variable electron energy: 25 – 500 MeV

BTF beam properties:

DETECTOR BEAM

slide-28
SLIDE 28

MENU 2013 –Rome, 2/10/2013

FT-Cal prototype test @ LNF BTF

FT-CAL BTF test results

  • Excellent linearity up to 4 GeV
  • Good

agreement

  • f

the experimental energy resolution with MC results for Ee>1.5 GeV

  • Low-energy MC-underestimated

noise contribution Measure @0°C

slide-29
SLIDE 29

MENU 2013 –Rome, 2/10/2013

Conclusions

  • Low Q2 electron scattering provides a high-flux of linearly polarized, quasi-real

photons: competitive and complementary to “real” photo-production experiments.

  • The Forward Tagger Facility in Hall B at Jefferson Laboratory is designed to

perform quasi-real photo-production experiments. Main physical motivation: spectroscopy

  • The Forward Tagger is made of 3 sub-detectors: FT-Cal, FT-Hodo, FT-Trck
  • Detector R&D completed
  • Design finalized
  • Construction in progress
  • Ready to take data with the first CLAS12 beam!
  • Tests from 16-channel FT-Cal prototype, both with cosmic rays and e- beam,

confirmed the detector operational principles, provided a first measure of the foreseen performances, and was used to tune MC parameters.

slide-30
SLIDE 30

MENU 2013 –Rome, 2/10/2013

Backup slides

slide-31
SLIDE 31

MENU 2013 –Rome, 2/10/2013

Neglect q-dependent terms due to EM current conservation:

Resulting amplitude is the product of two terms:

  • Emission of a quasi-real photon (m ~ 0) by the electron
  • Photoproduction on the proton of the final state pX

Photo-production amplitudes in the low Q2 framework

Reaction amplitude in the OPE approximation: Completeness relation for virtual-photon polarization:

slide-32
SLIDE 32

MENU 2013 –Rome, 2/10/2013

CLAS12 design specifications

slide-33
SLIDE 33

MENU 2013 –Rome, 2/10/2013

Forward Tagger integration in CLAS12