湯馬斯進動於實驗室座標系之研究

Thomas Precession and the Torque Equation from the Lab Frame Point of View

郭軒劭(Hsuan-Shao Kuo)

指導教授 ： 陳義裕

國立臺灣大學/理學院/物理研究所/碩士(2009年)

https://doi.org/10.6342/NTU.2009.03161

摘要

無資料

關鍵字

湯馬斯進動

並列摘要

Historically, Thomas precession came about as an attempt to explain why the thennew quantum theory involving electron spins could still correctly explain certain spectra
of anomalous Zeeman effect, despite a puzzling missing factor of 1/2 in a standard calculation.
In 1926, L.H.Thomas showed that people had overlooked a then-little-known relativistic kinematic effect in their calculations to resolve the puzzle.
Because Thomas precession can and should be checked against experiments in the lab, it seems reasonable and worthwhile to investigate how a magnetic dipole interacts with a given static electric field directly from the point of view of a lab observer.

並列關鍵字

Thomas Precession

參考文獻

[1] G.E. Uhlenbeck and S.A. Goudsmit, Naturwissenschaften 47, 953 (1925).

[2] S.A. Goudsmit and G. E. Uhlenbeck, “Spinning Electrons and the Structure of Spectra,” Nature, 117, 264-265, (1926).

[3] L.H. Thomas, “The motion of the spinning electron,” Nature, April 10, 514 (1926).

[4] L.H. Thomas, “The Kinematics of an Electron with an Axis,” Phil. Mag and J. Science, Ser. 7, 1-22 (1927).

[5] L. Silberstein, The Theory of Relativity, Chapter IV, MacMillan, 1914.