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Current and Recent Reviews* - 2 Avakian, L. N. Ananikyan, N. Ya. Ivanov, B. L. Berman, Y. Y. Ilieva, P. Nadel-Turonski, M. Mirazita, P. Rossi, K. Livingston, H. Avakian and V. D. Burkert - CAA: Determination of the Azimuthal Asymmetry in Deuteron Disintegration by Linearly Polarized Photons at Egamma = GeV Committee: Haiyan Gao, Eugene Pasyuk approved approved by Collaboration May 29, * If you want to modify this list send to
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Nuclear Physics Working Group MeetingMay 30, 2008 A110
Agenda
13:30-13:40 Jerry Gilfoyle, Update on reviews.13:40-14:05 Kawtar Hafidi, EG2 analysis update - I14:05-14:30 Larry Weinstein, Correlated pp to np pair ratios in 3He(e,e'pp)n14:30-14:55 Mikhail Osipenko, Update on inclusive scattering from E2a14:55-15:15 Break15:15-15:40 Lorenzo Zana, EG2 analysis update – II15:40-15:55 Steve Manly, Update on EG2 charged pion analysis15:55-16:20 Aji Daniel, Preliminary results on the nuclear dependence of the multiplicity ratios of neutral kaons16:20-16:45 Rakhsha Nasseripour, Photodisintegration of 4He to p and t
Current and Recent Reviews* - 1
Dan Protopopescu - Multipole Analysis of the Delta0(1232) in 3He Committee:Kyungseon Joo (Chair), Mike Vineyard, Mike Woodongoing
Hovhannes Baghdasaryan - 3He(e,e'pp)n AnalysisCommittee:Mike Vineyard (Chair), Dan Protopopescu, Steffen Strauchongoing
Rakhsha Nasseripour - Photodisintegration of 4He to p+tCommittee:Dave Ireland (Chair), Yelena Prok, Stephen Bueltmannongoing
Alex Vlasov – CAN: Source size measurements in the eHe -> e'p X reaction.Committee: Larry Weinstein (chair), Pavel Degtyarenko, Yordanka Ilievaongoing
Mikhail Osipenko, G. Ricco, S.Simula, M.Battaglieri, R. DeVita, M. Ripani, M. Taiuti, M. Anghinolfi – CAN: Moments of the nucleon structure function F2 with CLAS: Part III – nuclear target.Committee: Mike Dugger (chair), Tony Forest, Rakhsha Nasseripourongoing
* If you want to modify this list send email to [email protected]
Current and Recent Reviews* - 2
Avakian, L. N. Ananikyan, N. Ya. Ivanov, B. L. Berman, Y. Y. Ilieva, P. Nadel-Turonski, M. Mirazita, P. Rossi, K. Livingston, H. Avakian and V. D. Burkert - CAA: Determination of the Azimuthal Asymmetry in Deuteron Disintegration by Linearly Polarized Photons at Egamma = 1.1 - 2.3 GeVCommittee: Haiyan Gao, Eugene Pasyukapprovedapproved by Collaboration May 29, 2008.
* If you want to modify this list send email to [email protected]
Proposal Reviews for PAC33
• Medium Modification of , , – update of g7b– Mike Wood– Committee: Gabriel Nicelescu and Enzo DeSanctis– approved– conditionally approved by PAC33
• Direct Measurement of lifetime of heavy nuclei using fission fragment detection technique and CLAS with a real photon beam.
– L. Tang, A. Margaryan, B. Raue, and B. Hu– Committee: R.Schumacher, K.Hicks, B.Quinn– declined
L. Weinstein, Gordon 2004 5
Correlations in 3He(e,e’pp)nLarry Weinstein
Contradiction???
Subedi et al, Science (2008)
Ebeam <Q2> pn to pp ratio
Hall A / BNL
2 / ?? 18
2 GeV 0.8 3.14.7 GeV 1.5 4.5
Hall ABNL
Hall ABNL
np/2N
pp/2N
L. Weinstein, Gordon 2004 6
pp to pn resolution:pp/pn ratio increases with pair total
momentum Ptot
Theory: Wiringa, Schiavilla, Pieper and Carlson
Hall A: small Ptot less ppHall B: large Ptot more pp
Small Ptot pp pair in s-wave (no tensor) wave fn minimum at prel=400 MeV/c
300 < Prelative < 500 MeV/c
Prelim
inary
TensorCorrelations!
Hall A / BNL
L. Weinstein, Gordon 2004 7
3He(e,e’pp)n Summary•Analysis - follow the peaks
• pn < 250 MeV/c: pp ≈ 90o rescattering dominated• pN > 250 MeV/c
• Peaks at corners of Dalitz plots (T1, T2 < 0.2)• Cut pleading(perp) < 300 MeV/c: reduce leading N FSI
•Results:• NN pair is back-to-back• Small ptotal along q• Isotropic• Momentum distributions similar for 2.2 and 4.7 GeV• Moderate agreement with theory• pp to pn pair ratio increases with Ptotal
• 3N correlations???
•We have measured distorted correlated pairs!
Extraction of the Nuclear Structure Function F2 From E2a Data
Mikhail Osipenko
Structure functions agree with world data and at different beam energies. CLAS data dramatically increase kinematical coverage.
Carbon target
Extraction of the Nuclear Structure Function F2 From E2a Data
A Measurement of the Nuclear Transparency for r0; An Analysis of the Carbon+D2 Data
Lorenzo Zana
Analysis of Pion Production in eA – for “neutrino engineering”Melanie Day, Hyupwoo Lee, Steve Manly - Univ. of Rochester
Idea is to measure basic quantities (like differential pion cross sections) on different A to facilitate tuning of nuclear effects in neutrino experiment simulations - quite important for current/future high precision neutrino expts.
Have talked about it for a few years, so far only able to do “summer student” research on the problem.
Now have two neutrino grad students starting to do the dirty work necessary to actually make a measurement/paper.
Talking to experts on acceptance, radcorr, normalization, etc., hoping to avoid ‘reinventing the wheel’.
Making data plots with eg2 data (D2 and C), learning subtleties with GSIM, looking for pion generator/model, starting to look at normalization.
Nuclear Dependence of K0 Hadronization
Aji DanielQuark Propagation and Hadron Formation – Measure the space-time properties of hadron formation.
Focus on the formation time thf; the time for
the pre-hadron to evolve into a fully-dressed hadron (C, Fe, Pb targets).
Hermes resultsEG2 π+ preliminary
Nuclear Dependence of K0 Hadronization
Use the π+π- decay channel to reconstruct the K0.
Additional cuts on the pion vertex time and the trigger time
To do.
??
Significant Target dependence
Rakhsha Nasseripour,Barry Berman, Yordanka Rakhsha Nasseripour,Barry Berman, Yordanka IlievaIlieva
05/03/23 15Nuclear Physics WG Meeting
PHOTODISINTEGRATION of 4He to p + t
Reaction Mechanisms and Theoretical Calculations
One-body : proton or triton exchange
Two-body : two nucleon meson exchange and nucleon- nucleon rescattering
Three-body : meson double scattering
Background-Free Event Selection
Kinematics of real pt events require:
E(x) = 0 GeVP(x) = 0 GeV/cM(X)2 = 0
(GeV/c2)2
pt = 180 deg
Acceptance Corrections
Cross Sections (Energy Dependence)
One-body
Two-body
Three-body
Laget Model
We have extracted the cross sections for the We have extracted the cross sections for the photodisintegration of 4He to pt for photon energies photodisintegration of 4He to pt for photon energies above 0.4 GeV and proton scattering angles between above 0.4 GeV and proton scattering angles between 40 and 140 degrees. 40 and 140 degrees.
Comparison with Laget model confirms the importance Comparison with Laget model confirms the importance of the contribution of the three-body mechanisms at of the contribution of the three-body mechanisms at lowerlower photon energies and large angles.photon energies and large angles.
Analysis of systematic uncertainties is underway.Analysis of systematic uncertainties is underway.
Our analysis note is nearly completed.Our analysis note is nearly completed.
We request for an Analysis Review Committee.We request for an Analysis Review Committee.
05/03/23 Nuclear Physics WG Meeting 17
Summary