Abstract
The eigenstates of the phase operator are calculated for a two-mode radiation field subject to the condition that these be also the eigenstates of the operator corresponding to the difference q of the number of photons in the two modes. The phase distribution associated with such states has the form 1 [1 + F sin 2 ( θ 2 )] . In the special case q = 0, these eigenstates become identical to the two-mode squeezed vacuum.
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.
