Abstract
A rigorous quantum theory of optical NMR in atoms is developed in the coupling scheme J = L + S; F = J + I, where L, S and I are the orbital, spin electronic and nuclear spin quantum numbers, respectively. The optical NMR Hamiltonian is developed for a coupled state | LSJIFM F〉 in terms of products of 9 − j symbols, which are evaluated numerically. The optical NMR resonance condition is described in terms of the selection rule △ M F = 0, ±1 on the azimuthal quantum number of F, the net angular momentum. The theory shows clearly that the original NMR resonance line is shifted and split into several lines by the applied circularly polarised laser of optical NMR.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
