How does COMSOL arrive at its rotating potential term for the Hamiltonian in rotating frame?

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Hello,

I'm trying to understand how COMSOL arrives at the term (Which it shows you in COMSOL) to add onto the Hamiltonian if you solve the Schrödinger equation in a rotating reference frame.

Does anyone know where I can look this stuff up? There's nothing in the semiconductor manual about it and the page in the documentation is very meek https://doc.comsol.com/6.2/docserver/#!/com.comsol.help.semicond/semicond_ug_schrodinger.8.11.html?highlight=rotating%25E2%2590%25A4frame


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