Virtual Compton Scattering measurements in the nucleon resonance region
A. Blomberg, H. Atac, N. Sparveris, M. Paolone, P. Achenbach, M. Benali, J. Beričič, R. Böhm, L. Correa, M. O. Distler, A. Esser, D. Flay, H. Fonvieille, I. Fri… 展开作者
A. Blomberg, H. Atac, N. Sparveris, M. Paolone, P. Achenbach, M. Benali, J. Beričič, R. Böhm, L. Correa, M. O. Distler, A. Esser, D. Flay, H. Fonvieille, I. Friščić, Y. Kohl, H. Merkel, U. Müller, Z. E. Meziani, M. Mihovilovic, J. Pochodzalla, A. Polychronopoulou, B. Pasquini, M. Schoth, F. Schulz, S. Schlimme, C. Sfienti, S. Sirca, A. Weber
We report on new measurements of the electric Generalized Polarizability (GP) of the proton $α_E$ in a kinematic region where a puzzling dependence on momentum transfer has been observed, and we have found that $α_E = (5.3 \pm 0.6_{stat} \pm 1.3_{sys})~10^{-4} fm^3$ at $Q^2=0.20~(GeV/c)^2$. The new measurements, when considered along with the rest of the world data, suggest that $α_E$ can be described by either a local plateau or by an enhancement in the region $Q^2=0.20~(GeV/c)^2$ to $0.33~(GeV/c)^2$. The experiment also provides the first measurement of the Coulomb quadrupole amplitude in the $N \rightarrow Δ$ transition through the exploration of the $p(e,e'p)γ$ reaction. The new measurement gives $CMR = (-4.4 \pm 0.8_{stat} \pm 0.6_{sys})~\%$ at $Q^2=0.20~(GeV/c)^2$ and is consistent with the results from the pion electroproduction world data. It has been obtained using a completely different extraction method, and therefore represents a strong validation test of the world data model uncertainties.
Virtual Compton Scattering and Nucleon Generalized Polarizabilities
本文综述了低能区核子$γ^* N \to N γ$的虚康普顿散射(VCT)。我们回顾了与广义极化率(GP)和模型预测这些观测值的理论形式主义。我们提出的GP提取方法,在实验中使用的方法:基于低能量定理的色散关系和形式主义的方法。然后我们回顾了实验结果,重点介绍了最近的质子广义极化率实验数据所带来的进展,并对低能质子广义极化率领域的研究进行了展望。
我们研究了最近的深虚康普顿散射(DVCS)的数据在一个双重参数化的广义部分子分布(GPD)。这种参数化允许量化的最大数量的信息,可以从DVCS数据中提取,在一个“精粹”的功能。我们提出了一个“零步”模型,后者完全基于前向夸克密度,提供了一个参数的DVCS振幅的虚部的预测。结果表明,$e p \to e p γ$光束螺旋度不对称的体效应可以在这样的模型内理解。
Photon-nucleon entanglement in Compton scattering at low and high energies
Physics Department, Brookhaven National Laboratory(布鲁克海文国家实验室物理系);RIKEN BNL Research Center, Brookhaven National Laboratory(理化学研究所布鲁克海文研究中心);Université Paris-Saclay - CEA - IRFU(巴黎萨克雷大学-法国原子能和替代能源委员会-核物理研究所);Center for Frontiers in Nuclear Science, Stony Brook University(纽约州立大学石溪分校核科学前沿中心)