Abstract
A semiclassical representation is introduced to the quantum theory of a strong field, based on a possibility of defining the semiclassical evolution operator in quantum theory, whose effect on the operators of a field and a quantum system transforms them into the solutions of an appropriate semiclassical problem. This representation enables one to go, in a simple way, from a quantum problem to a corresponding semiclassical one, and to use equations of the semiclassical theory as a calculations apparatus in quantum theory and to determine the applicability limits of the semiclassical theory. The possibilities of using the semiclassical representation introduced are illustrated by its use in nonrelativistic quantum electrodynamics.
Sign-in/Register to access full text options 
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.
