'Polarized 3' presentation slideshows

Single Spin Asymmetries and Transverse Structure of the Nucleon

Single Spin Asymmetries and Transverse Structure of the Nucleon. Jian -ping Chen ( ??? ) , Jefferson Lab, Virginia, USA Seminar @ USTC, Hefei, China, July 9, 2013. Introduction Recent SSA Results from JLab New Preliminary SSA Results from JLab

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Polarized Targets and Physics Program

Polarized Targets and Physics Program. Jian -ping Chen, Jefferson Lab JLab high luminosity polarized targets workshop, June 18-19, 2010. Introduction Progress in the last decade 12 GeV program and needs How to meet the needs. Introduction to Spin and Polarized Targets.

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Prospects in neutron transverse spin study with a polarized 3 He Target at 12 GeV JLab

Prospects in neutron transverse spin study with a polarized 3 He Target at 12 GeV JLab. (. A Third Joint meeting of Division of Nuclear Physics of American Physical Society and the Japanese Physical Society Oct 13-17, 2009

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A Proposal of a Polarized 3 He ++ Ion Source with Penning Ionizer for JINR

A Proposal of a Polarized 3 He ++ Ion Source with Penning Ionizer for JINR. N.N. Agapov, Yu.N. Filatov, V.V. Fimushkin, L.V. Kutuzova, V.A. Mikhailov, Yu.A. Plis, Yu. V. Prokofichev, V.P. Vadeev Joint Institute for Nuclear Research, Dubna, Russia.

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The first measurement of neutron Transversity using a transversely polarized 3 He target

The first measurement of neutron Transversity using a transversely polarized 3 He target. Yi Qiang Duke University for the Workshop on Hadron Physics in China and Opportunities with 12 GeV JLab July 31, 2009. Outline. Overview of leading twist TMDs Jefferson Lab Experiment E06-010

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Polarized 3 He Target for 12 GeV Experiments J. P. Chen, February 12, 2013, Hall A Meeting

Polarized 3 He Target for 12 GeV Experiments J. P. Chen, February 12, 2013, Hall A Meeting. Introduction Target performance for 6 GeV experiments 12 GeV experiments and requirements Upgrade plan and status. Principle for Polarizing Targets. Polarization Brute Force:

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Polarized 3 He Target for 12 GeV Experiments J. P. Chen, February 12, 2013, Hall A Meeting

Polarized 3 He Target for 12 GeV Experiments J. P. Chen, February 12, 2013, Hall A Meeting. Introduction Target performance for 6 GeV experiments 12 GeV experiments and requirements Upgrade plan and status. Principle for Polarizing Targets. Polarization Brute Force:

326 views • 23 slides

SoLID SIDIS Update

SoLID SIDIS Update. Zhiwen Zhao University of Virginia For SoLID Collaboration Hall A Collaboration Meeting 201 3 /12/17. SoLID ( Solenoidal Large Intensity Device). Lumi 1e 37 /cm 2 /s (open geometry) 3D hadron structure TMD (SIDIS on both neutron and proton) (3 EXPs, 1 LOI)

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A proposal for a polarized 3 He ++ ion source with the EBIS ionizer for RHIC.

A proposal for a polarized 3 He ++ ion source with the EBIS ionizer for RHIC. A.Zelenski, J,Alessi, E.Beebe, A.Pikin BNL M.Farkhondeh, W.Franklin, A. Kocoloski, R.Milner, C. Tschalaer, E.Tsentalovich MIT-Bates E.Hughes Caltech SPIN 2004, Trieste. Motivation.

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E06-010 / E06-011 Transversity Experiments Overview, Manpower and Safety

E06-010 / E06-011 Transversity Experiments Overview, Manpower and Safety. Readiness Review, March 19, 2007. Goal of the transversity experiments Requirements of the transversity experiments Collaboration and manpower Safety issues.

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Development of a Polarized 3 He Target at RCNP

Development of a Polarized 3 He Target at RCNP. Youhei Shimizu RCNP, Osaka University. Collaborators. RCNP, Osaka University : Y. Shimizu , K. Hatanaka, Y. Sakemi, A. Tamii, H.P. Yoshida, M. Uchida, Y. Shimbara, K. Fujita, Y. Tameshige, H. Matsubara CNS, University of Tokyo :

353 views • 17 slides

An attempt toward dynamic nuclear polarization for liquid 3 He

17/Nov./2005 @ PST2005. An attempt toward dynamic nuclear polarization for liquid 3 He. Takahiro Iwata Yamagata University. 1. Motivation of the study 2 ? Polarizing 3 He in dense form 3. DNP for liquid He3 3 ? Doping with free radical 4. ESR signals 5. Summary.

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Spin Correlation Parameter C yy of p + 3 He Elastic Backward Scattering at Intermediate Energy

Spin Correlation Parameter C yy of p + 3 He Elastic Backward Scattering at Intermediate Energy. Youhei Shimizu RCNP, Osaka University. Collaborators. RCNP, Osaka University : Y. Shimizu , K. Hatanaka, Y. Sakemi, A. Tamii, H.P. Yoshida,

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The status of 3 He Relaxation Time Measurement at ~400mK

The status of 3 He Relaxation Time Measurement at ~400mK. Q. Ye, D. Dutta, H. Gao, W. Zheng, X. Zhu Duke University R. Golub, P. Huffman, F. Dubose NC State University May 20, 2008. Outline. Experimental Apparatus 2007 Summer Results Modifications to the MC & acrylic cell

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Polarized 3 He Neutron Spin Filter Development at ORNL

Polarized 3 He Neutron Spin Filter Development at ORNL. Hal Lee, Dennis Rich Instrument Development Group, Neutron Facilities Development Division Oak Ridge National Laboratory Oak Ridge, TN 37831, USA. What we have done in the past.

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HALL-A STATUS REPORT

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Why Studying n-DVCS ?

Eric Voutier. Why Studying n-DVCS ?. 0 because F 1 (t) is small. 0 because of cancelation of u and d quarks. Sensitivity of the difference of polarized cross sections to the angular momentum of quarks. n-DVCS gives access to the least known and constrained GPD, E. Eric Voutier.

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JLab Spin Experiments

JLab Spin Experiments. Completed/on-going: n ( 3 He), both g 1 and g 2 , 0.02 GeV 2 < Q 2 < 5 GeV 2 p/d, g 1 , 0.02 GeV 2 < Q 2 < 5 GeV 2 p/d, g 2 , Q 2 =1.3 GeV, 2 GeV 2 < Q 2 < 5 GeV 2 Spin experiments to be done at 6 GeV: g 2 p at low Q 2 (not practical with 12 GeV)

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Two-photon Exchange as a Laboratory for Nucleon Structure Studies

Two-photon Exchange as a Laboratory for Nucleon Structure Studies. The entire response of the nucleon is contained in the two-photon box. A y : Measure the target SSA using quasi-elastic scattering from vertically polarized 3 He. E05-015 ,

176 views • 4 slides