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Optics Letters

Amplitude squeezing of light by means of a phase-sensitive fiber parametric amplifier

Dmitry Levandovsky, Michael Vasilyev, Prem Kumar

Published Jul 15, 1999• 65 citations
Publisher

Abstract

We experimentally demonstrate generation of bright sub-Poissonian light by means of parametric deamplification in a phase-sensitive fiber amplifier that is based on a balanced nonlinear Sagnac interferometer. On direct detection, the photocurrent noise falls below the shot-noise limit by (0.6 +/- 0.2) dB (1.4 dB when corrected for detection losses). To observe the noise reduction we employed a scheme that used two orthogonally polarized pulses to cancel the noise that arises from the predominantly polarized guided-acoustic-wave Brillouin scattering in the fiber. We also present a simplified semiclassical theory of quantum-noise suppression by this amplifier, which is found to be in good agreement with the experimental results.

DOI
10.1364/ol.24.000984

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We experimentally demonstrate generation of bright sub-Poissonian light by means of parametric deamplification in a phase-sensitive fiber amplifier that is based on a balanced nonlinear Sagnac interferometer. On direct detection, the photocurrent noise falls below the shot-noise limit by (0.6 +/- 0.2) dB (1.4 dB when corrected for detection losses). To observe the noise reduction we employed a scheme that used two orthogonally polarized pulses to cancel the noise that arises from the predominantly polarized guided-acoustic-wave Brillouin scattering in the fiber. We also present a simplified semiclassical theory of quantum-noise suppression by this amplifier, which is found to be in good agreement with the experimental results.
Sub-Poissonian pulses of light are generated by means of traveling-wave optical parametric deamplification. Upon direct detection the quantum noise on the deamplified pulses is measured to be below the shot-noise limit by as much as 0.5\ifmmode\pm\else\textpm\fi{}0.2 dB (11\ifmmode\pm\else\textpm\fi{}4 %). The parametric-gain dependence of the measured Fano factor---direct-detection noise as a fraction of the shot-noise limit---agrees with the quantum theory of the amplifier when diffraction effects are taken into account.
Near-degenerate four-wave parametric mixing in an optical fiber couples fluctuations in signal and idler frequency bands in such a way that the noise at a particular optical phase is reduced while that in an orthogonal phase quadrature is amplified. We have performed experiments on this effect and explained our results in terms of a theory which incorporates a nonlinear dispersion effect. The nonlinear dispersion alters the mathematical character of the solutions and limits the effective interaction length. For relatively low frequency shifts (<100 GHz) and 100 m of fiber, the heterodyne detected optical noise can be reduced by 5 dB in the squeezed quadrature. Theory predicts that this parametric interaction should reduce the noise level below the standard quantum limit. In a realistic fiber, phase noise due to guided acoustic wave Brillouin scattering (GAWBS) dominates the quanturn noise and cannot be reduced by four-wave mixing. Narrow gaps in the GAWBS noise can be engineered into special fibers. At the frequencies of these gaps, the noise level indeed can be squeezed below the quantum limit.
We have clearly demonstrated the parametric deamplification of electromagnetic vacuum fluctuations in a traveling wave geometry using a single-mode optical fiber.1 The minimum detected noise level was 12.5 ± 0.5% below the noise level produced by an incandescent source at the same photocurrent. Noise levels below the standard quantum limit appeared in two 9-MHz wide frequency bands centered at 45 and 56 MHz. At other frequencies, noise due to guided acoustic wave Brillouin scattering overwhelmed the squeezing, even at 2 K. Stimulated Brillouin oscil­lation was avoided by dividing the pump wave into many frequency components with a phase modulator. The theory of squeezed state generation and detection with such a multifrequency pump is discussed as are the phenomena which limit the noise suppression by this technique.