氢原子O(α)阶引力张量-单极矩

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Xiangdong Ji, Jinghong Yang, Yizhuang Liu
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The result is <h:math xmlns:h=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><h:msub><h:mi>τ</h:mi><h:mi>H</h:mi></h:msub><h:mo>/</h:mo><h:msub><h:mi>τ</h:mi><h:mn>0</h:mn></h:msub><h:mo>−</h:mo><h:mn>1</h:mn><h:mo>=</h:mo><h:mfrac><h:mrow><h:mn>4</h:mn><h:mi>α</h:mi></h:mrow><h:mrow><h:mn>3</h:mn><h:mi>π</h:mi></h:mrow></h:mfrac><h:mrow><h:mo stretchy=\"false\">(</h:mo><h:mi>ln</h:mi><h:msup><h:mi>α</h:mi><h:mn>2</h:mn></h:msup><h:mo>−</h:mo><h:mn>0.028</h:mn><h:mo stretchy=\"false\">)</h:mo></h:mrow><h:mo>=</h:mo><h:mo>−</h:mo><h:mn>3.06</h:mn><h:mo>×</h:mo><h:msup><h:mn>10</h:mn><h:mrow><h:mo>−</h:mo><h:mn>2</h:mn></h:mrow></h:msup></h:math> where <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:msub><l:mi>τ</l:mi><l:mn>0</l:mn></l:msub><l:mo>=</l:mo><l:msup><l:mi>ℏ</l:mi><l:mn>2</l:mn></l:msup><l:mo>/</l:mo><l:mn>4</l:mn><l:msub><l:mi>m</l:mi><l:mi>e</l:mi></l:msub></l:math> is the leading-order moment. 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The result is <h:math xmlns:h=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><h:msub><h:mi>τ</h:mi><h:mi>H</h:mi></h:msub><h:mo>/</h:mo><h:msub><h:mi>τ</h:mi><h:mn>0</h:mn></h:msub><h:mo>−</h:mo><h:mn>1</h:mn><h:mo>=</h:mo><h:mfrac><h:mrow><h:mn>4</h:mn><h:mi>α</h:mi></h:mrow><h:mrow><h:mn>3</h:mn><h:mi>π</h:mi></h:mrow></h:mfrac><h:mrow><h:mo stretchy=\\\"false\\\">(</h:mo><h:mi>ln</h:mi><h:msup><h:mi>α</h:mi><h:mn>2</h:mn></h:msup><h:mo>−</h:mo><h:mn>0.028</h:mn><h:mo stretchy=\\\"false\\\">)</h:mo></h:mrow><h:mo>=</h:mo><h:mo>−</h:mo><h:mn>3.06</h:mn><h:mo>×</h:mo><h:msup><h:mn>10</h:mn><h:mrow><h:mo>−</h:mo><h:mn>2</h:mn></h:mrow></h:msup></h:math> where <l:math xmlns:l=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><l:msub><l:mi>τ</l:mi><l:mn>0</l:mn></l:msub><l:mo>=</l:mo><l:msup><l:mi>ℏ</l:mi><l:mn>2</l:mn></l:msup><l:mo>/</l:mo><l:mn>4</l:mn><l:msub><l:mi>m</l:mi><l:mi>e</l:mi></l:msub></l:math> is the leading-order moment. 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引用次数: 0

摘要

在量子电动力学(QED)中,我们计算了氢原子基态O(α)阶动量-电流密度Tij的引力张量-单极矩。得到τH/τ0−1=4α3π(lnα2−0.028)= - 3.06×10−2,其中τ0= 2/4me为一级矩。次一级修正的物理原理类似于著名的能级兰姆位移。2024年由美国物理学会出版
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Gravitational tensor-monopole moment of the hydrogen atom to order O(α)
We calculate the gravitational tensor-monopole moment of the momentum-current density Tij in the ground state of the hydrogen atom to order O(α) in quantum electrodynamics (QED). The result is τH/τ01=4α3π(lnα20.028)=3.06×102 where τ0=2/4me is the leading-order moment. The physics of the next-to-leading-order correction is similar to that of the famous Lamb shift for energy levels. Published by the American Physical Society 2024
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来源期刊
Physical Review D
Physical Review D 物理-天文与天体物理
CiteScore
9.20
自引率
36.00%
发文量
0
审稿时长
2 months
期刊介绍: Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics. PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including: Particle physics experiments, Electroweak interactions, Strong interactions, Lattice field theories, lattice QCD, Beyond the standard model physics, Phenomenological aspects of field theory, general methods, Gravity, cosmology, cosmic rays, Astrophysics and astroparticle physics, General relativity, Formal aspects of field theory, field theory in curved space, String theory, quantum gravity, gauge/gravity duality.
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