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| age | 25 | |
| visits | member for | 4 months |
| seen | May 18 at 18:44 | |
| stats | profile views | 4 |
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Jan 11 |
revised |
Alkali atom in oscilating electromagnetic field short answer added |
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Jan 11 |
awarded | Scholar |
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Jan 11 |
accepted | Alkali atom in oscilating electromagnetic field |
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Jan 11 |
comment |
Alkali atom in oscilating electromagnetic field Thank you for the nice explanation! The rotating wave approximation (when applicable) indeed helps to get rid of the counter-rotating terms. Having looked into books that deal with linearly polarized almost-resonant light, I didn't expect to find counter-rotating terms as separate matrix elements, and this eventually led me to the faulty assumption that these terms should not appear in the Hamiltonian at all. |
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Jan 10 |
awarded | Editor |
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Jan 10 |
revised |
Alkali atom in oscilating electromagnetic field added 220 characters in body |
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Jan 10 |
comment |
Alkali atom in oscilating electromagnetic field Thank you for your input, Emilio! I am quite convinced that I am calculating 3j symbols correctly. Values of reduced matrix elements $\langle \eta^\prime\parallel d\parallel\eta\rangle$ should be real. Initial matrix elements would be real only if the corresponding electric dipole operator matrix elements were real, which I believe is not the case. The Wigner-Eckart theorem tells us that for $\Delta m=\pm 1$ transition the only nonzero component of $\hat{\mathbf{d}}$ is for either $q=+1$ or $-1$. And this corresponds to complex $x,y$ components in the Cartesian basis. |
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Jan 8 |
awarded | Student |
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Jan 8 |
asked | Alkali atom in oscilating electromagnetic field |