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来自晶格量子色动力学的质子-质子聚变和氚β衰变

Proton-Proton Fusion and Tritium β Decay from Lattice Quantum Chromodynamics.

作者信息

Savage Martin J, Shanahan Phiala E, Tiburzi Brian C, Wagman Michael L, Winter Frank, Beane Silas R, Chang Emmanuel, Davoudi Zohreh, Detmold William, Orginos Kostas

机构信息

Institute for Nuclear Theory, University of Washington, Seattle, Washington 98195-1550, USA.

Kavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106, USA.

出版信息

Phys Rev Lett. 2017 Aug 11;119(6):062002. doi: 10.1103/PhysRevLett.119.062002. Epub 2017 Aug 10.

Abstract

The nuclear matrix element determining the pp→de^{+}ν fusion cross section and the Gamow-Teller matrix element contributing to tritium β decay are calculated with lattice quantum chromodynamics for the first time. Using a new implementation of the background field method, these quantities are calculated at the SU(3) flavor-symmetric value of the quark masses, corresponding to a pion mass of m_{π}∼806  MeV. The Gamow-Teller matrix element in tritium is found to be 0.979(03)(10) at these quark masses, which is within 2σ of the experimental value. Assuming that the short-distance correlated two-nucleon contributions to the matrix element (meson-exchange currents) depend only mildly on the quark masses, as seen for the analogous magnetic interactions, the calculated pp→de^{+}ν transition matrix element leads to a fusion cross section at the physical quark masses that is consistent with its currently accepted value. Moreover, the leading two-nucleon axial counterterm of pionless effective field theory is determined to be L_{1,A}=3.9(0.2)(1.0)(0.4)(0.9)  fm^{3} at a renormalization scale set by the physical pion mass, also agreeing within the accepted phenomenological range. This work concretely demonstrates that weak transition amplitudes in few-nucleon systems can be studied directly from the fundamental quark and gluon degrees of freedom and opens the way for subsequent investigations of many important quantities in nuclear physics.

摘要

首次利用格点量子色动力学计算了决定(pp→de^{+}ν)聚变截面的核矩阵元以及对氚(β)衰变有贡献的伽莫夫-泰勒矩阵元。通过背景场方法的新实现方式,在夸克质量的(SU(3))味对称值下计算了这些量,对应于(m_{π}∼806 MeV)的π介子质量。发现在这些夸克质量下,氚中的伽莫夫-泰勒矩阵元为(0.979(03)(10)),在实验值的(2σ)范围内。假设矩阵元的短程关联两核子贡献(介子交换流)仅微弱依赖于夸克质量,如同在类似磁相互作用中所见,计算得到的(pp→de^{+}ν)跃迁矩阵元导致在物理夸克质量下的聚变截面与其当前公认值一致。此外,在由物理π介子质量设定的重整化标度下,无π介子有效场论的主导两核子轴向反项被确定为(L_{1,A}=3.9(0.2)(1.0)(0.4)(0.9) fm^{3}),也在公认的唯象范围内相符。这项工作具体表明,少核子系统中的弱跃迁振幅可以直接从基本的夸克和胶子自由度进行研究,并为后续核物理中许多重要量的研究开辟了道路。

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