The proton form factor measurements at Jefferson Lab, past and future

被引:0
|
作者
Vina Punjabi
机构
[1] Norfolk State University,
来源
关键词
Form Factor; Electromagnetic Form Factor; Recoil Proton; Pauli Form Factor; Nucleon Electromagnetic Form Factor;
D O I
暂无
中图分类号
学科分类号
摘要
Use of the double-polarization technique to obtain the elastic nucleon form factors has resulted in a dramatic improvement of the quality of two of the four nucleon electromagnetic form factors, GEp and GEn. It has also changed our understanding of the proton structure, having resulted in a distinctly different Q2-dependence for both GEp and GMp, contradicting the prevailing wisdom of the 1990’s based on cross section measurements, namely that GEp and GMp obey a “scaling” relation μGEp ∼ GMp. A related consequence of the faster decrease of GEp revealed by the Jefferson Lab (JLab) polarization results was the disappearance of the early scaling F2/F1 ∼ 1/Q2 predicted by perturbative QCD. In three experiments, GEp(1), GEp(2) and GEp(3), in Halls A and C at JLab, the ratio of the proton’s electromagnetic elastic form factors, GEp/GMp, was measured up to four momentum transfer Q2 of 8.5 GeV2 with high precision, using the recoil polarization technique. The initial discovery that the proton form factor ratio measured in these three experiments decreases approximately linearly with four-momentum transfer, Q2, for values above ∼ 1 GeV2, was modified by the GEp(3) results, which suggests a slowing down of this decrease. There is an approved experiment, GEp(5), to continue these measurements to 15 GeV2. A dedicated experimental setup, the super bigbite spectrometer (SBS), will be built for this purpose. It will be equipped with a new focal plane polarimeter to measure the polarization of the recoil protons. In this presentation, I will review the status of the proton elastic electromagnetic form factors, mention succinctly a number of theoretical approaches to describe results and show some features required for the future GEp(5) experiment.
引用
收藏
页码:163 / 166
页数:3
相关论文
共 50 条
  • [41] Future Perspectives on Baryon Form Factor Measurements with BES III
    Schonning, Karin
    Li, Cui
    XIITH QUARK CONFINEMENT AND THE HADRON SPECTRUM, 2017, 137
  • [42] Automated path length and M56 measurements at Jefferson Lab
    Hardy, D
    Tang, J
    Legg, R
    Tiefenback, M
    Crofford, M
    Krafft, GA
    PROCEEDINGS OF THE 1997 PARTICLE ACCELERATOR CONFERENCE, VOLS 1-3: PLENARY AND SPECIAL SESSIONS ACCELERATORS AND STORAGE RINGS - BEAM DYNAMICS, INSTRUMENTATION, AND CONTROLS, 1998, : 2265 - 2267
  • [43] Analysis of Deeply Virtual Compton Scattering data at Jefferson Lab and proton tomography
    R. Dupré
    M. Guidal
    S. Niccolai
    M. Vanderhaeghen
    The European Physical Journal A, 2017, 53
  • [44] The Q(weak) Experiment: A measurement of the proton's weak charge at Jefferson Lab
    Myers, K. E.
    NUOVO CIMENTO C-COLLOQUIA AND COMMUNICATIONS IN PHYSICS, 2012, 35 (04): : 171 - 175
  • [45] Results and future perspectives of the neutron spin structure studies at Jefferson Lab
    Deur, A
    CZECHOSLOVAK JOURNAL OF PHYSICS, 2002, 52 : C251 - C259
  • [46] Unpolarized proton DVCS at 10.6 GeV with CLAS12 at Jefferson Lab
    Christiaens, Guillaume
    27TH INTERNATIONAL NUCLEAR PHYSICS CONFERENCE (INPC2019), 2020, 1643
  • [47] Analysis of Deeply Virtual Compton Scattering data at Jefferson Lab and proton tomography
    Dupre, R.
    Guidal, M.
    Niccolai, S.
    Vanderhaeghen, M.
    EUROPEAN PHYSICAL JOURNAL A, 2017, 53 (08):
  • [48] Proton Form Factor Measurements Using Polarization Method: Beyond Born Approximation
    Pentchev, Lubomir
    SIXTH INTERNATIONAL CONFERENCE ON PERSPECTIVES IN HADRONIC PHYSICS, 2008, 1056 : 357 - 364
  • [49] Experimental Validation of the Born Approximation in Proton Form Factor Measurements With Polarization Method
    Pentchev, Lubomir
    SPIN PHYSICS, 2009, 1149 : 589 - 592
  • [50] Measurements of the deuteron electric and magnetic form factors at the Jefferson Laboratory
    Petratos, GG
    NUCLEAR PHYSICS A, 2000, 663 : 357C - 360C