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E07-006 :Status Report Nucleon-Nucleon Short-Range Correlation (NN SRC)
on He4 target
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Outline [General SRC] • What is Nucleon-Nucleon Short
Range Correlation(NN-SRC)?• Why is NN-SRC interesting?• What has been done?• Our Unique Experiment Setting.• What we have from Spring 2011
running period?• Analysis Progress
• Experiment/Analysis Approaches– Inclusive X(e,e’)– Double coincident X(e,e’p)– Triple coincident X(e,e’pN)– (new approach) Double
coincident on the recoil partner X(e,e’N_recoil) (backward nucleon)
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WHAT IS NUCLEON-NUCLEON SHORT RANGE CORRELATION(NN-SRC)?
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What is Nucleon-Nucleon Short Range Correlation (NN-SRC)?
• the phenomena are when the wave functions of the two nucleons are strongly overlapping
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WHY IS NN-SRC INTERESTING?5
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NN-SRC is interesting because …
• The nuclear shell model can only predict 60% of the spectral function. Long range correlation can only provide a 20% contribution. The short range correlation is believed to contribute the remaining 20%.
6
Target MassSP
ECTR
OSC
OPI
C ST
REN
GTH
L. Lapikas, Nucl. Phys. A553 (1993) 297.
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NN-SRC is interesting because …
• The measurement of nucleon momentum distributions for various nuclei yields a similar high momentum tail. Along with the shell model, the existence of NN-SRC pairs within the nuclei is believed to explain this phenomenon.
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NN-SRC is interesting because …
• The study of the NN-SRCs within the nucleus also provides more insight into cold, dense nuclear matter such as that found in neutron stars.
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WHAT HAS BEEN DONE?9
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Inclusive MeasurementCLAS A(e,e’) data
• The observed scaling means that the electrons probe the high-momentum nucleons in the 2N-SRC phase, and the scaling factors determine the per-nucleon probability of the 2N-SRC phase in nuclei with A>3 relative to 3He
10K. Sh. Egiyan et al., Phys. Rev. C 68 (2003) 014313.
r(A,3He) = a2n(A)/a2n(3He)
x = Q2
2M>1.5
Q2 > 1.4 [GeV/c]2
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Result (e,e’) and (e,e’p) and (e,e’pN) from E01-015
• 80 +/- 5% single particles moving in an average potential– 60 – 70% independent single
particle in a shell model potential – 10 – 20% shell model long range
correlations• 20 +/- 5% two-nucleon short-
range correlations– 18% np pairs– 1% pp pairs– 1% nn pairs (from isospin symmetry)
• Less than 1% multi-nucleon correlations
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12
Correlated Pair Fractions from 12C R. Subedi et al., Science 320 (2008) 1476.
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13
OUR UNIQUE EXPERIMENT
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14
Customized (e,e’pN) Measurement
A pair with “large” relativemomentum between the nucleons
and small center of mass momentum
Relative to the Fermi-sea level ~ 250 MeV/c
• High Q2 to minimize MEC (1/Q2) and FSI
• x>1 to suppress isobar contributions
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15
Experiment E07-006 vs E01-015 Missing momentum 400 – 800 MeV/c Tensor to Repulsive
Core
E01-015 E07-006XB >1, Q2 = 2 [Gev/c]2 XB >1, Q2 = 2
[Gev/c]2
300 – 600 MeV/c 400 – 800 MeV/c
Tensor Force Tensor to Repulsive core
Target – 12C Target – 4He(Less FSI)
BigBite and HAND BigBite with MWDCsUpgraded HAND(new lead wall)
Pushing Limits of NN Potential– Long range attraction– Short range repulsion
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E07-006: 4He(e,e’pN)pn SRC• 4He Target
– Dense Nuclear Matter– Mean Feild & Exact
Calculations• Pm from 400 – 800 MeV 3 Kinematic setting: 500,650 & 750 MeV/c This reduce to two kinematic
for (e,e’N_recoil) , BigBite is at 97 degree and 92 degree.
Pmiss [MeV/c]
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WHAT WE HAVE FROM OUR EXPERIMENT RUN-PERIOD?
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Production dataProduction period March 15 - April 13, 2011
May 11-12, 2011
Beam 4.46 GeV
Current 4 uA
Target He4 20 cm loop
HRS, Left Arm (fixed): 20.3 deg, 3.6 GeV/c
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Production dataKinematic Setting Right HRS BigBite Cumulative Charge
Kin 1 :(p_miss = 500 MeV/c)
33.5 deg, 1.38 GeV/c
Angle: 97 degCurrent: 518 A
1.6 C With 0.7 C has no major problems
Kin 2 :(p_miss = 650 MeV/c)
29.0 deg, 1.31 GeV/c
Angle: 97 degCurrent: 518 A
1.67 C
Kin 3:(p_miss = 750 MeV/c
24.5 deg, 1.196 GeV/c
Angle: 92 degCurrent: 518 A
2.98 C
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ANALYSIS PROGRESS…
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Calibration Phase
21
Detector What has been done?
Ongoing What Not? Problems/Concerns
Beam Line - BPM- BCM
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Calibration Phase
22
Detector What has been done?
Ongoing What Not? Problems/Concerns
Left HRS: as electron spectrometer
- Vetex, theta,phi optics matrix
- Vdc t0 - S2
scintilator Time
- Cherenkov- Lead Glass
- Momentum optics matrix
- ½ of Kinematics 1 has overflow of the Cerenkov., ..Only use the Lead Glass detector as Particle Identification (PID)
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Calibration Phase
23
Detector What has been done?
Ongoing What Not? Problems/Concerns
Right HRS: as proton spectrometer
- Vdc t0 - S2 & S1
scintillators relative time
- optics matrix
- S2 time by itself
other detectors that not applicable for proton PID are not calibrated
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Calibration Phase
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Detector What has been done?
Ongoing What Not? Problems/Concerns
BigBite - MWDC t0 calibration
- E & dE TDC & ADC calibration
Optics N/A
Neutron Extraction Code aiming for the maximum identify neutron
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LEFT HRS OPTIC CALIBRATION28
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Vertex Calibration
• Vertex calibration with 13 carbon foils with 25 mm separation (300 mm total length)
• Achieve the resolution of 2.5 to 3.9 mm
• Show the possibility of using high density optic foils.
29
Phi (rad)
Verte
x (m
)
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Vertex Reconstruction for 20 cm He4 target
Before Calibration New Calibration
30Vertex z (m) Vertex z (m)
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Vertex Reconstruction for 20 cm He4 target
Before Calibration (cut window) New Calibration (cut window)
31Vertex z (m) Vertex z (m)
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Vertex Reconstruction for 20 cm He4 target
32
New Calibration (cut window)
Verte
x z
(m)
Phi (rad)
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In-plane & out-of-plane angles Calibration
33Sieve Y (m)
Sie
ve X
(m)
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In-plane & out-of-plane angles Calibration
34
Sieve Y (m)
Sie
ve X
(m
)
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S2 Timing Calibration
35
[Define]TOF = S2Time – pathlength/(beta*c)
TOF (ns)
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Cherenkov Calibration
36
After calibration
Before calibration
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Pion Rejecter Calibration
Before CalibrationEnergy Deposit in Pb Glass Detector
37
Layer 2 Energy [MeV]
Laye
r 1 E
nerg
y [M
eV]
Layer 2 Energy [MeV]
Laye
r 1 E
nerg
y [M
eV]
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RIGH HRS OPTIC CALIBRATION38
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Right Beta distribution
39
Beta calculation from beta = (pathlength)/(time*c)
between S1 and S2 Scintilators
Proton at 0.78
Pion at 0.99
He4 at 0.2
Deuteron at 0.53
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BIGBITE CALIBRATION40
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BigBite Calibration
• Calibration of the dE vs E energy deposit
41
Deuteron
Proton
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Trigger planesEnergy deposit with taging electron
Energy deposit with coincidence timing with electron
42
E plane (channel)
dE p
lane
(ch
anne
l)
E plane (channel)
dE p
lane
(ch
anne
l)
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BigBite Momentum from Analytical Model
With tagging electron With coincidence timing with electron
43Momentum (GeV/c) Momentum (GeV/c)
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NEUTRON CALIBRATION
44
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HAND calibration
ADC channel
* Pedestals alignment
* Threshold determination
* TDC alignment
* Time walk correction
* Position calibration
* TOF calibration for elastic scattering
* Neutron detection efficiency
ADC Histogram (with TDC>0) divided by ADC Histogram with no TDC cut
ADC Channel
Correspond to ~4 MeVee (Calibrated with known energy deposit)
Pedestals Alignment
Before after
Threshold determination
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Time walk correction
Data is fitted to:
Sigma = 1.2 ns
Sigma = 0.6 ns
Position [cm] Position:* Black – data after calibration.* Red – uniform distribution from -50 to 50 (cm) with Gaussian resolution of 10 cm.
Position Calibration
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Neutron detection efficiency We have d(e,e'pn) coincidence data at two kinematic settings : * Pmiss between 0.22 – 0.38 GeV/c * Pmiss between 0.38 – 0.52 GeV/c
In progress
Pmiss: 0.22 – 0.38 GeV/c
Pmiss 0.38 – 0.52 GeV/c:
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PRELIMINARY RESULTS48
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Two Aimed Results• 1. The triple coincident result:
– Ratio (e,e’pp)/(e,e’p)– Ratio (e,e’pn)/(e,e’p)– Ratio (e,e’pp)/(e,e’pn)
• 2. the double coincident with backward (recoiled) nucleon.– Absolute cross-section
(e,e’N_recoiled)– Ratio
(e,e’p_recoiled)/(e,e’n_recoiled)
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Preliminary Triple Coincident
• The P_miss distribution of each kinematic. 50
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• Spokespersons:• Shalev Gilad (MIT)• Douglas Higinbotham (JLab)• Eli Piasetzky (Tel Aviv)• Vincent Sulkosky (MIT)• John Watson (Kent State)
• Postdocs:• Aidan Kelleher (MIT)• Charles Hanretty (Uva)• Ran Shneor (Tel Aviv)
• Graduate Students:• David Anez (Saint Mary’s)• Or Chen (Tel Aviv)• Igor Korover (Tel Aviv)• Navaphon (Tai) Muangma (MIT)• Larry Selvy (Kent State)• Zhihong Ye (Uva)
Acknowledgements
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The END
Follow our analysis at http://hallaweb.jlab.org/experiment/
E07-006/analysis_page.html53
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Electron PID using Lead Glass Detector
After calibration we have the clear separation of the electron from pion. At our kinematic setting for the Left HRS, we rarely have the contamination from the pion, i.e., 97% electron production rate.
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Current Status
• Electron PID- Separating
electron from pion
• Two possible requirements for Election PID:– Create Signal above background in
Cherenkov detector (NOT USE)– Deposit large amount of energy in (two-
layer) lead glass where (Aprox.) E/p = 1.
55