Timeline for Time Reserval Symmetry Operator on Spin Orbit Coupling
Current License: CC BY-SA 4.0
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| Apr 3, 2022 at 17:40 | comment | added | Kieran | @Mauricio Thank you for the reply. In other words, if I multiply the spin-orbit coupling term in the followings: $$e^{i\pi J_y}\langle d_{xy}\uparrow|\xi L\cdot\sigma|p_{z}\downarrow\rangle$$; where $$e^{i\pi J_y}$$ is the time reversal operator, this term should change the sign. Am I correct? If so, how to choose $J_y$, the y-component of the angular momentum operator, for different term? I think that this operator varies with different orbital $p_z$,$d_{xy}$. Thank you. | |
| Mar 17, 2022 at 9:41 | comment | added | Mauricio | Spin orbit does not change sign under time reversal that's the whole point of Kramers theorem. | |
| Mar 8, 2022 at 17:40 | history | asked | Kieran | CC BY-SA 4.0 |