3. Multipolar Gauge & Length form for interaction hamiltonian


Length form VS. Velocity form
           In approximated treatments of atom-radiation interaction (ARI), the controversy over whether to use a velocity form (as obtained from the Coulomb gauge) or  a length form (as obtained from the Multipolar gauge) was resolved by Kobe in 1979 for identical-particle systems on the basis of gauge invariance. In quantum coherent control of different-particle systems, it is still an issue of which form to choose. Although the validity of the Multipolar gauge treatment with the electric dipole approximation (EDA) is controversial, it is a proper treatment. This paper shows that, for a three-atom system, the transition rate between quantum states induced by the electromagnetic field is the same for the two forms in a resonant case with a local Hamiltonian. The paper also shows that there is a transition rate difference between the two gauges for nonlocal Hamiltonians. Reasons for a preference to the length form over the velocity form will be explained based on gauge-invariant property of the approximate molecular Hamiltonian.
       Link: My documentation on this topic
             My poster on this topic

Multipolar gauge with nonadiabatic terms
          To be able to control the chemical reaction, people have shown great interest on the atom-radiation interaction. Different derivations have been established for different gauges applied. On the basis of  gauge invariance property, Donald Kobe advocated the use of the Multipolar gauge in 1979. However in the special case of atom-diatiom system with laser, general theory has not been established. What's more, the nonadiabatic cases have interested a lot of people. It is also a challengle to include the nonadiabatic terms in the atom-radiation interaction.
        Link: My documentation on this topic


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