首页> 外文期刊>Nuclear Physics, A: Journal Devoted to the Experimental Study of the Fundamental Constituents of Matter and Their Actions >Compton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q(4))
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Compton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q(4))

机译:质子,中子和氘核在质子,中子和氘核上的康普顿散射对O(Q(4))

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We study Compton scattering in systems with A = 1 and 2 using chiral perturbation theory up to fourth order. For the proton we fit the two undetermined parameters in the O(Q(4)) gammap amplitude of McGovern to experimental data in the region omega,root less than or equal to 180 MeV, obtaining a x(2)/d.o.f. of 133/113. This yields a model-independent extraction of proton polarizabilities based solely on low-energy data: alpha(p) = (12.1 +/- 1.1(stat.)) (+0.5)(-0.5)(theory) and beta(p) = (3.4 +/- 1.1(stat.)) (+0.1)(-0.1) (theory), both in units of 10(-4) fm(3). We also compute Compton scattering on deuterium to O(Q(4)). The gammad amplitude is a sum of one- and two-nucleon mechanisms, and contains two undetermined parameters, which are related to the isoscalar nucleon polarizabilities. We fit data points from three recent gammad scattering experiments with a x(2)/d.o.f. = 26.6/20, and find alpha(N) = (13.0 +/- 1.9 (stat.)) (+3.9)(-1.5) (theory) and a beta(N) that is consistent with zero within sizable error bars. (C) 2004 Elsevier B.V. All rights reserved.
机译:我们使用至多四阶的手性扰动理论研究A = 1和2的系统中的康普顿散射。对于质子,我们将McGovern的O(Q(4))gammap振幅中的两个未确定参数拟合到omega,root t 小于或等于180 MeV区域中的实验数据,得出x(2)/d.o.f。 133/113。仅基于低能量数据即可得出质子极化率的模型独立提取:alpha(p)=(12.1 +/- 1.1(stat。))(+0.5)(-0.5)(理论)和beta(p) =(3.4 +/- 1.1(stat。))(+0.1)(-0.1)(理论),均以10(-4)fm(3)为单位。我们还计算了氘在O(Q(4))上的康普顿散射。 gamgam振幅是一个和两个核子机制的总和,并且包含两个不确定的参数,这些参数与等比例的核子极化率有关。我们使用x(2)/d.o.f拟合来自三个最近的gammad散射实验的数据点。 = 26.6 / 20,并找到alpha(N)=(13.0 +/- 1.9(stat。))(+3.9)(-1.5)(理论)和一个beta(N),在相当大的误差线内与零保持一致。 (C)2004 Elsevier B.V.保留所有权利。

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