2016
DOI: 10.1364/oe.24.028383
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Creation and measurement of broadband squeezed vacuum from a ring optical parametric oscillator

Abstract: We report a 65 MHz-bandwidth triangular-shaped optical parametric oscillator (OPO) for squeezed vacuum generation at 860 nm. The triangle structure of our OPO enables the round-trip length to reach 45 mm as a ring cavity, which provides a counter circulating optical path available for introducing a probe beam or generating another squeezed vacuum. Hence our OPO is suitable for the applications in high-speed quantum information processing where two or more squeezed vacua form a complicated interferometer, like … Show more

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Cited by 58 publications
(34 citation statements)
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“…We consider the case where such a field has a much larger linewidth than the cavity mode. Indeed, a squeezing bandwidth of up to ∼ GHz has been experimentally demonstrated via optical parametric amplification [38][39][40]. Because the linewidth is ∼ MHz for typical optical cavities, we can think of this cavity drive as a squeezed reservoir.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…We consider the case where such a field has a much larger linewidth than the cavity mode. Indeed, a squeezing bandwidth of up to ∼ GHz has been experimentally demonstrated via optical parametric amplification [38][39][40]. Because the linewidth is ∼ MHz for typical optical cavities, we can think of this cavity drive as a squeezed reservoir.…”
mentioning
confidence: 99%
“…Moreover, the cavity mode can be squeezed typically using, e.g., a periodicallypoled KTiOPO 4 (PPKTP) crystal [48][49][50]. In order to generate a squeezed-vacuum reservoir, we can also use a PPKTP crystal with a high-bandwidth pump, so the squeezing bandwidth of up to ∼ GHz [38,39] is possible.…”
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confidence: 99%
“…Such a scheme encodes two real numbers from a continuous Gaussian distribution and therefore it has much higher capacity per time interval than a discrete encoding. Due to recent developments in the field of quantum optics, both coherent and displaced squeezed states can be generated with sufficient purity [31,32]. The signal state prior to modulation can be therefore described by the diagonal covariance matrix γ B = diag[V s , 1/V s ], where V s is the variance of the squeezed quadrature, here and further, without loss of generality, it is assumed to be the X quadrature (covariance matrix for a coherent state reduces to a 2 × 2 unity matrix).…”
Section: Qkd Protocolmentioning
confidence: 99%
“…In the following, we demonstrate the squeezing-induced noise, i.e., thermal noise and two-photon correlation, can be suppressed by employing a squeezed field to drive the cavity. In view of a highbandwidth squeezed field (up to GHz), which has been realized in experiments [51,52], it can be regarded as a squeezed reservoir due to a relatively small linewidth of typical optical cavity mode. Therefore, we assume that the cavity mode is coupled to a squeezed thermal reservoir with a squeezing parameter r e and phase θ e .…”
Section: Appendix: Effective Master Equationsmentioning
confidence: 99%