2002
DOI: 10.1088/1464-4266/4/1/302
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Characteristics of bright-squeezed light produced in a below-threshold optical parametric oscillator

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Cited by 8 publications
(2 citation statements)
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“…In an OPO the only input is the pump field, the input to the squeezed mode is a vacuum state and hence a squeezed vacuum mode is generated. If a coherent input seed field is introduced in an OPA, the squeeze operator is acting on a coherent state and a bright squeezed mode is generated [113]. The phase difference between the pump and seed input fields determines the argument of the complex squeeze parameter θ and the angle in quadrature space along which the output state will be squeezed.…”
Section: Cavity Qedmentioning
confidence: 99%
“…In an OPO the only input is the pump field, the input to the squeezed mode is a vacuum state and hence a squeezed vacuum mode is generated. If a coherent input seed field is introduced in an OPA, the squeeze operator is acting on a coherent state and a bright squeezed mode is generated [113]. The phase difference between the pump and seed input fields determines the argument of the complex squeeze parameter θ and the angle in quadrature space along which the output state will be squeezed.…”
Section: Cavity Qedmentioning
confidence: 99%
“…It should be noted that in the previous related works [20,34,36,37,39,40] the relevant amplitude expansion contained only a single quadratic term, namely, the first one according to (14). However, as (14) suggests, the extra quadratic term may significantly contribute to the field amplitude, especially at the nearthreshold oscillation, where the pump amplitude value may be far stronger than the generated amplitudes: A A p j 0 (j = 1, 2).…”
Section: Quadratic Approximationmentioning
confidence: 95%