2019
DOI: 10.1364/ol.44.001789
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Dependence of the squeezing and anti-squeezing factors of bright squeezed light on the seed beam power and pump beam noise

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Cited by 17 publications
(7 citation statements)
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“…Modern sources of squeezed light typically use optical parametric oscillators or amplifiers (OPOs and OPAs); by placing the non-linear medium in an optical cavity the strength of the non-linear interaction is enhanced and the spectral properties of the generated squeezed state can be tuned. These OPO/A cavities can take the form of external Fabry-Pérot or ring cavities, or fully monolithic or semimonolithic designs using reflective coatings applied directly to the non-linear crystal end surfaces [110][111][112]. Depending on the input modes to the cavity, two broad classes of squeezed states are generated: squeezed vacuum and bright squeezed states, these are illustrated in Figure 4.…”
Section: Cavity Qedmentioning
confidence: 99%
“…Modern sources of squeezed light typically use optical parametric oscillators or amplifiers (OPOs and OPAs); by placing the non-linear medium in an optical cavity the strength of the non-linear interaction is enhanced and the spectral properties of the generated squeezed state can be tuned. These OPO/A cavities can take the form of external Fabry-Pérot or ring cavities, or fully monolithic or semimonolithic designs using reflective coatings applied directly to the non-linear crystal end surfaces [110][111][112]. Depending on the input modes to the cavity, two broad classes of squeezed states are generated: squeezed vacuum and bright squeezed states, these are illustrated in Figure 4.…”
Section: Cavity Qedmentioning
confidence: 99%
“…1. The laser source of our experiment is a home-made single-frequency Nd:YVO4 laser at 1064 nm with the output power of 2.5 W. The laser preparations, including spatial-mode improvement, intensity noise suppression, polarization purification and second harmonic generation, are similar to our earlier experiments presented in Refs [29,45,46]. Our OPA is a semi-monolithic cavity consisting of a piezoactuated concave mirror and a PPKTP crystal with the dimensions of 1mm 2mm 10mm  .…”
Section: Methodsmentioning
confidence: 95%
“…The noise variances of measured PAR phase are limited by initial squeezing factor and system loss. It is worth noting that the parametric amplification process (for the generation of quadrature phase squeezed state) intensifies the noise coupling between the seed and pump field, which usually results in the degradation of the squeezing factor [42]. As the pump factor is increased, the noise coupling enhances.…”
Section: Figmentioning
confidence: 99%