電子の磁気モーメントを精密計算(Calculating the Electron’s Magnetic Moment)

ad

2025-07-08 カリフォルニア工科大学 (Caltech)

カリフォルニア工科大学(Caltech)の研究者らは、電子の磁気モーメントをこれまでで最も高精度に計算することに成功した。磁気モーメントは量子電磁気学(QED)の基本予測の一つであり、実験値と理論値の一致は標準理論の正確さを示す指標とされる。今回の成果では、超精密なQED補正項を含む新たな計算手法を用い、実験との誤差が極めて小さい理論値が導出された。これにより、標準模型の限界を探る手段としての電子の磁気モーメントの重要性が改めて強調され、新たな物理の発見に向けた一歩と位置付けられている。

<関連情報>

電子の磁気モーメントはどれくらい異常か? How Anomalous is the Electron’s Magnetic Moment?

Charles T. Sebens
Foundations of Physics  Published:07 June 2025
DOI:https://doi.org/10.1007/s10701-025-00846-1

Abstract

The electron’s spin magnetic moment is ordinarily described as anomalous in comparison to what one would expect from the Dirac equation. But, what exactly should one expect from the Dirac equation? The standard answer would be the Bohr magneton, which is a simple estimate of the electron’s spin magnetic moment that can be derived from the Dirac equation either by taking the non-relativistic limit to arrive at the Pauli equation or by examining the Gordon decomposition of the electron’s current density. However, these derivations ignore two effects that are central to quantum field theoretic calculations of the electron’s magnetic moment: self-interaction and mass renormalization. Those two effects can and should be incorporated when analyzing the Dirac equation, to better isolate the distinctive improvements of quantum field theory. Either of the two aforementioned derivations can be modified accordingly. Doing so yields a magnetic moment that depends on the electron’s state (even among z-spin up states). This poses a puzzle for future research: How does the move to quantum field theory take you from a state-dependent magnetic moment to a fixed magnetic moment?

1701物理及び化学
ad
ad
Follow
ad
タイトルとURLをコピーしました