Nonclassical states of light induced via measurement in a bimodalsystem

• URL: http://arxiv.org/abs/2504.08515v1
• Date: Fri, 11 Apr 2025 13:27:13 GMT
• Title: Nonclassical states of light induced via measurement in a bimodalsystem
• Authors: R. Chakrabarti, S. V. Iyengar, B. V. Jenisha,
• Abstract summary: We investigate generation of nonclassical photon states via conditional measurement process in a two mode coupled waveguide.<n>An initial two mode squeezed state undergoes a unitary evolution governed by the interaction Hamiltonian for a specified time.<n>The nonclassicality of the post-measurement states obtained here may be textitcontrolled by varying the interaction strength and the time span of interaction between the modes.
• Score: 0.0
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: We investigate generation of nonclassical photon states via conditional measurement process in a two mode coupled waveguide. Interaction of the fields takes place in a waveguide beamsplitter due to the overlap between normal modes supported therein. A quadratic Hamiltonian of two degrees of freedom describes the hopping interaction. An initial two mode squeezed state undergoes a unitary evolution governed by the interaction Hamiltonian for a specified time. Following this the bipartite state is subjected to a projective measurement that detects $n$-th Fock state in one subsystem. The post-measurement excitation rendered in the residual subsystem depends on the prior time of interaction between the modes as well as the interaction strength. The Wigner quasiprobability distribution of an arbitrary post-selection state is computed. Its nonclassicality is examined via the negativity of the Wigner distribution. The sub-Poissonian nature of the photon statistics is revealed by the Mandel parameter. The dynamically generated squeezing is evidenced in the post-measurement state. In the ultrastrong coupling regime the parity even and odd states display markedly \textit{different} nonclassical properties. The nonclassicality of the post-measurement states obtained here may be \textit{controlled} by varying the interaction strength and the time span of interaction between the modes.

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