Physics with low energy recoil detector and options for instrumentation for the CLAS12 S. Stepanyan (JLAB) CLAS12 European Workshop February 25-28, 2009, Genova, Italy
Dec 31, 2015
Physics with low energy recoil detector and options for instrumentation for the CLAS12
S. Stepanyan (JLAB)
CLAS12 European Workshop
February 25-28, 2009, Genova, Italy
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
2
Few physics topics with low energy recoil ( ) detector
• neutron structure
• nuclear structure (see also K. Joo’s talk)
• meson spectroscopy
Options for a recoil detector
• RTPC
• LPMWPC&SSD
4A
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Neutron target and accessible physics
PDF at large x d/u at large x quark-hadron duality on neutron neutron elastic scattering neutron DVCS
S. Bueltman et al., E12-06-113
Free neutrons decay in 15 min Can we explore the structure of the neutron if all we have are
neutrons bound in nuclei? – nuclear model uncertainties
Low energy spectator tagging can be a solution for a neutron target:
nnBeBe
ndH
npH
s
s
89
3
2
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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d/u ratio at x 1
F2n
F2p
14d /u
4 d /u
d
u
4 F2n F2p 1
4 F2n F2p
F2n/F2p = F2d/F2p -1
???
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Modifications to Simple Spectator Picture
Final State Interactions
“BoNuS”
Binding Effects
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Spectator Tagging with BoNuS RTPC
2/
ˆ;,
D
SSSSSS M
qpEpEp
pn MD ES ,p S ;
n 2 S
W 2 M 2 2M Q2
22
222
)2(2*
)(2*
QMM
QqpEMppqpW
S
nsDnnn
x Q 2
2 pnq
Q 2
2M (2 S )
*
E = 4.223 GeV
e
p
n
<Q2> = 1.19 (GeV/c)2
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Coherent DVCS Nuclear GPDs - partonic structure of nuclei, momentum and spatial distribution of quarks in nuclei,
generalized EMC effect
Incoherent DVCS bound nucleon GPDs – nuclear medium effects,
modification with respect to free nucleon ones
DVCS on nuclei
Coherent DVCS Incoherent DVCS
Both will require low energy recoil detector
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Coherent and incoherent were not cleanly separated.
Nuclear DVCS
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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For nucleon DVCS:
CLAS experiment E08-024 (K. Hafidi et al.)
m{H 4 He}
e{H 4 He}
ALU () 0()
1()2() 3()(2 2 )
4He nucleusFC I H
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Meson spectroscopy
(1232)N(1520)
N(1680)
Strong kinematical cuts and a complex PWA are required
Production on hydrogen - physics background from associated baryon resonance production
, N*
CLAS/g6: p’n++-
a2(1320)
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Spectroscopy in coherent production on nuclei
Method to eliminate the baryon background
044
33
33
MHeHe
MHHe
MHeH
All three charged modes can be studied using gas targets 3H, 3He, and 4He
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Example: coherent production on 4He
eHHe 404*
eHHe 404 '*
);(' 0
0 andwith
Scattering off a spin and isospin zero target works as a spin and parity filter
JLAB experiment E07-009, Stepanyan et al.
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Coherent production of 0 and 0’ off 4He
Only C=-1 -exchanges is allowed, Natural Parity Exchange (NPE)
22
0
AAAd
d
C
),(Im212 0
2/1max
0 1
LL
L
L
DLLA
;0;00 AA
),(Im212 101
2/1max
1
LL
L
DLLA
22
2
2111 sinsin)1cos5(
2
7
2
1cos53
FDPd
d
C
The helicity of the produced state will be that of the incoming photon, =, production of 0 (0’) in S-wave is forbidden
Test for above assumptions
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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CLAS12 central detector
Silicon Vertex Tracker
Scintillator Counters, t=50ps
5T SC Solenoid Magnet
Low (200 MeV/c) energy protons in CLAS12 CD (M. Ungaro, GEMC)
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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CLAS12 Central detector
Protons Deuterons
Specialized detector is needed for a broad physics program requiring low energy recoil detection
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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BoNuS* RTPC**
*BoNuS = Barely off-shell Nucleon Scattering**RTPC = Radial Time Projection Chamber
BoNuS
Region
VIPs
0.07 0.2 GeV/c
D (r p )
2
Gas Electron Multiplier
Drift Region
Helium/DME at 80/20 ratio
Readout pads and electronics
7 atm D2 gas
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Performance and limitations of BoNuS RTPC
dE/dx from charge along the tracke- reconstructed in CLAS & RTPC
z
=8mm
=4º=1.4ºReasonable 3-vector reconstruction
Reasonable PID for a proton
Low rate of DAQ - ~500Hz
Poor PID for high mass fragments – gain uniformity of GEM pads
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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BoNuS-II (for EG6 run in October)
Lightweight (carbon-foam composite structure) rungs for stress-free, self support of GEMs – to avoid “wrinkles”
Target region - new cell – ID 4mm, 30m thick wall
Ground and cathode foils, each 6m thick
Open, 2 geometry – only 80% is accessible due to the GEM and readout pad sizes
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Expected performance of BoNuS-II
Expected PID with fully calibrated RTPCBetter gain uniformity – better PID: new GEM foils stress free support calibration system (-source and
elastic scattering)
Lower momentum threshold (250 MeV for ’s)
thinner target walls
Increased DAQ rate - 0.5 kHz to 5 kHz new RCUs, crate, backplane … work
is done at INFN Genova (R. De Vita, M. Battaglieri, S. Minutoli)
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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DAQ with new Readout Control Unit board
Lo
cal M
onito
ra
nd
Co
ntr
ol BOARD
Controller
RCU
DCS ( 1 MB/s )
DDL ( 200 MB/s )
Front-end bus( 200 MB / s )
Control Network(I2C-serial link)
Bu
s c
on
tro
ller
( c
on
f. &
R/O
)
FEC128 ch
1
1
2
2
13
13
DCS int.(Ethernet)
DAQ int.(DDL-SIU)
Trigger int.(TTC-RX)
FEC128 ch
FEC128 ch
FEC128 ch
FEC128 ch
FEC128 ch
Rx - PASA - ALTRO
DE
TE
CT
OR
TTC optical Link
(Clock, L1 and L2 )
Data Proc.and MemoryTx
Triggerand Timing
circuit
Max event rate 7 kHz
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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LPAC&SSD* (NIKHEF NIM A409, 1998)
* Low-pressure avalanche chamber and silicon strip detectors
MeV
H 3.2
2H 4.2
3H 4.9
3He 11
4He 13
H 2H 3H 3He 4He
8.8 12 14 31 35 MeVIsobutane@ 7 mbar
SiX E or E, x
SiY E or E, y
Sci E
AC E, t(t=100ps), y
Entrance foil – 1m
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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LPMWPC (JLAB FF detector NIM A426, 1999)
Two windowless gas proportional counters with three electrodes, operating as a parallel plate (wire planes) avalanche counter
Silicon strip detectors to measure full energy
Options for running the chamber with helium, helium/heptane (99%/1%), or helium/hydrogen (86%/15%) are under studies (YerPhI/Idaho)
Detector was developed by YerPhI group for detection of fission fragments for studies of the absolute photofission cross sections at MAX-lab (Lund, Sweden) and for hypernuclear experiments in Hall C at JLAB
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Test of LPMWPC in Hall B Two symmetric arms placed on top and bottom of the beam centerline
The inner chambers active area - 10.5 x 21cm2
Distance of the anode plane from the beam line - 3 cm.
The outer chambers - 21 x 21 cm2
Target - 209Bi with a thickness of 2 mg/cm2.
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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RTPC and LPMWPCBoNuS RTPC LPMWPC&SSD
Rate High High
Background Insensitive to MIP Insensitive to MIP
Momentum resolution Dp/p~20%, full trajectory fitting
Two point position recopnstruction
Minimum energy ~6 MeV for Defined by target, can be ~1 MeV for
Efficiency ~100% ~100%
Time resolution None ~200ps
Use in the trigger No Yes
Solid targets No, high accidental rates, long drift time
Yes, good for heavier fragments
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Summary
Broad physics program, ranging from nucleon and nuclear structure to meson spectroscopy, can be accessed with CLAS12 and a low energy recoil detector
Exploration of some of these physics topics is started with CLAS and BoNuS RTPC
2nd generation RTPC will have much improved characteristics for PID and data rate (3rd generation detector for CLAS12 can have ~2 azimuthal coverage)
Option with LPMWPC must be carefully studied, specially for the detection of -s and the heavier fragments from solid targets
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
2727
CLAS12
cGeVPth /9.4
cGeVPth /7.2
Low Threshold Cherenkov Counters
High Threshold Cherenkov Counter (HTCC)
Pre-shower calorimeters
Electromagnetic calorimeters
CLAS12 Torus
Drift Chambers
TOF Counters
Central Detector
CLAS12 Solenoid
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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S. Liuti & S. K. Taneja PRC72, 2005
Gomez et al., PRD49, 1994
Medium Modification
4He/D
• The deviations from unity is mostly due to convolutions with k.
• The asymmetry ratio for DVCS enhances the EMC effect.
EMC effect
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Electroproduction at “0” degrees [photoproduction]
Reaction ep’pX at 5.76 GeV
(e1-6 and e1-DVCS experiments)Missing transverse momentum distribution for |MX|2<0.1 GeV
Invariant mass of 2 photon pairs in the reaction ep’p(e’)1.0
22
X
yX
X
xX
P
P
P
P
Data were taken with loosely defined electron trigger
CLAS12 European Workshop February 25-28, 2009, Genova, Italy
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Reaction ep’p(e’) andep’p(e’)
CLAS e1-6 CLAS DVCS
Note:- data were taken with unfavorable trigger conditions- transferred momentum squared, |t|>0.2 (GeV/c)2 (proton momentum >0.4 GeV/c) - spectra contain the baryon background