It is considered the non-symmetric perfectly solvable Hamiltonian describing a system of a fermion in the external magnetic field that couples to a harmonic oscillator via some pseudo-hermitian interaction.
We highlight all of
the original Mandal and Jaynes-Cummings Hamiltonians' properties. Under the
combined action of the parity operator and the time-reversal operator, we show
that the Mandal Hamiltonian is non hermitian and non invariant. It has been
proven that the Mandal Hamiltonian is pseudo-hermitian with regard to and also
[1,2], even if the previous properties are not satisfied. As a result, the
original Jaynes-Cummings Hamiltonian is shown to be hermitian.
After expressing
the Mandal and Jaynes-Cummings Hamiltonians in the position and impulsion
operators, we show that they are both exact solvable, comparable to the direct
approach to invariant vector spaces described in Refs [3,4].
Author(S) Details
Ancilla Nininahazwe
Institut de Pédagogie Appliquée, Université du Burundi, Bujumbura, Burundi.
View Book:- https://stm.bookpi.org/NRAMCS-V1/article/view/6548
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