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Journal of Experimental and Theoretical Physics

Micromaser operation in correlated atoms

В. Н. Горбачев, Andrew I. Trubilko

Published Oct 1, 2002• 0 citations
Publisher

Abstract

Stimulated emission of two-level atoms in a high-Q cavity is considered under conditions when pumping produces correlated many-atomic states. Based on the many-body problem, a kinetic equation is obtained for the Glauber–Sudarshan probability, which describes the field in the Fokker–Planck approximation. The statistics of light in this approximation are determined by the atomic correlation functions of the order of no higher than the second. The noise of light is found in the regime of micromaser operation for two types of pumping producing the initial separable states with a classical correlation and entangled states. It is shown that the presence of the initial diatomic correlation enhances the intensity noise. The entangled state of atoms is found from which nonclassical light is generated with a steady-state phase and noise, which can be almost completely suppressed in the low-frequency spectral region.

DOI
10.1134/1.1520593

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Stimulated emission of two-level atoms in a high-Q cavity is considered under conditions when pumping produces correlated many-atomic states. Based on the many-body problem, a kinetic equation is obtained for the Glauber–Sudarshan probability, which describes the field in the Fokker–Planck approximation. The statistics of light in this approximation are determined by the atomic correlation functions of the order of no higher than the second. The noise of light is found in the regime of micromaser operation for two types of pumping producing the initial separable states with a classical correlation and entangled states. It is shown that the presence of the initial diatomic correlation enhances the intensity noise. The entangled state of atoms is found from which nonclassical light is generated with a steady-state phase and noise, which can be almost completely suppressed in the low-frequency spectral region.
Two-mode generation of light in a system of N identical relaxation-free atoms placed in a resonator is considered on the basis of the derived controlling Fokker-Planck equation for the Glauber-Sudarshan quasiprobability. Under steady-state conditions, a state of modes is formed with nonclassical correlation characterized by sub-Poison statistics of photons and leading to complete suppression of shot noise. Being an entangled pair, these sub-Poisson modes can be used as a quantum channel for teletransmission of light. In contrast to the standard Einstein-Podolskly-Rosen (EPR) channel, the recipient can reproduce only correlation functions of the intensity of an unknown state.
When pumping produces atomic coherence on working levels or atomic polarization two-level atom can generate the light without inversion. In such systems one- and two-photon generation of the light is considered for the laser and micromaser operation. Using Lamb-Scully model generalized for coherent pumping statistics of the light is considered. Two-photon laser operation is found to be phase squeezed and perfect noise reduction can be achieved. In maser a set of steady state of subpoissian photon statistics is found. For these states the noise reduction up to 60 percent can be obtained if inversion is zero. Phase squeezing in micromaser is found.
Two micromasers are coupled by sharing a common pump beam. A stream of excited atoms first passes through one micromaser and then enters a second one. The steady state of the second micromaser exhibits a second threshold at θ2= 2. The second threshold is accompanied with a jump of π in the phase of the second micromaser. For higher values of the pump parameter θ new branches of the steady-state intensity keep appearing. In certain parameter regions the phase of the second micromaser locks to that of the first and exhibits correlated emission laser-like noise quenching. In other regions the intensity fluctuations exhibit antibunching. The approach to steady state is also highly nonclassical. There are sharp jumps of magnitude π in the phase of the second micromaser and the intensity tends to overshoot before they settle to their steady-state value. In this transient regime the system exhibits phase noise squeezing.