Abstract
In the present work we treat problems of propagation by expanding the field operators in terms of mode operators associated with definite frequencies. Since a mode with a definite frequency is connected to energy eigenket with eigenvalue ħω, the Hamiltonian of such mode is of the form with no interaction term. and are the creation and annihilation operators for the flux of photons in a cross section A, and time T and is the number operator for this flux of photons.
© 1994 IEEE
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