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Annual Meeting Optical Society of America

Twin beams, squeezed light, and their uses

E. Giacobino, Jerome C. Mertz, Claude Fabre, Serge Reynaud, A. Heidmann

Published Jan 1, 1991• 0 citations
Publisher

Abstract

In recent years, several experiments have established the optical parametric oscillator (OPO) as a practical source of highly correlated twin beams. These beams have an intensity difference noise substantially below the associated shot noise, for noise frequencies within the OPO cavity bandwidth. They present the additional feature of being laserlike and intense, making them convenient for experimental applications. Refinements on our OPO characteristics and photodiode efficiencies have yielded a reduction of the noise power in the intensity difference of 86% below the shot noise level.1 A first use of twin beams is the production of a single light beam having an intensity squeezed noise. This can be achieved by monitoring the intensity of one beam with a photodiode and using this information to control the intensity fluctuations of the second beam with an electrooptic modulator.2 Other applications to high sensitivity spectroscopic measurements such as linear and nonlinear absorption or dispersion can now be considered for practical use.

DOI
10.1364/oam.1991.mbb1

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In recent years, several experiments have established the optical parametric oscillator (OPO) as a practical source of highly correlated twin beams. These beams have an intensity difference noise substantially below the associated shot noise, for noise frequencies within the OPO cavity bandwidth. They present the additional feature of being laserlike and intense, making them convenient for experimental applications. Refinements on our OPO characteristics and photodiode efficiencies have yielded a reduction of the noise power in the intensity difference of 86% below the shot noise level.1 A first use of twin beams is the production of a single light beam having an intensity squeezed noise. This can be achieved by monitoring the intensity of one beam with a photodiode and using this information to control the intensity fluctuations of the second beam with an electrooptic modulator.2 Other applications to high sensitivity spectroscopic measurements such as linear and nonlinear absorption or dispersion can now be considered for practical use.
It has been recently shown theoretically1 and experimentally2 that nondegenerate optical parametric oscillators generate above threshold intense and highly correlated twin beams. More precisely, the noise on the difference between the intensities of the two beams is well below the shot noise for noise frequencies inside the cavity bandwidth. An application of this quantum correlation is to measure the intensity of one beam and use this information to correct the fluctuations of the other beam by optoelectronic means (photodiode, amplifier, and electrooptic modulator). The correction may be applied either on the pumping beam (feedback correction) or directly on the twin beam itself (feed-forward correction).
We investigated the intensity noise spectra of a single beam of a pump-enhanced continuous-wave optical parametric oscillator (OPO), which was used to generate quantum-correlated twin beams, as a function of the pump power. With a triply (pump-, signal-, and idler-) resonant cavity, the oscillation threshold of our OPO was 8.5±1.3 mW and the measured slope conversion efficiency was 0.72±0.02. Twin beams with a power of 240 mW were generated at a pump power of 350 mW. The relaxation oscillation frequencies, which depend on the pump power, were observed when the pump power of the OPO was 12.5–28 mW. The experimental results confirm the predicted increase in OPO relaxation frequency with pump power. We experimentally inferred squeezing of the single-beam intensity, for the first time to our knowledge, by exploiting the nature of quantum noise that is dependent on loss.
Nondegenerate optical parametric oscillators generate above-threshold signal and idler beams that have intensity fluctuations correlated at the quantum level (twin beams). We describe what is to our knowledge the first high-sensitivity spectroscopy experiment using twin beams emitted by a cw optical parametric oscillator: a very weak two-photon absorption signal, in the 10(-7) range, is recorded on the 4S(1/2)-5S(1/2) transition of atomic potassium with a noise background that is reduced by 1.9 dB with respect to the shot-noise limit of the light used in the experiment.
We investigated the intensity noise spectra of the single beam of a pump-enhanced continuous-wave (cw) optical parametric oscillator (OPO), which was used to generate quantum correlated twin beams, as a function of the pump power. With a triply (pump-, signal-, and idler-) resonant cavity, the oscillation threshold of our OPO was about 8.5+/-1.3 mW and the measured slope conversion efficiency was 0.72+/-0.02. A twin beams with power of 240 mW were generated at pump power of 350 mW. The relaxation oscillation frequencies, which depend on the pump power, were observed when the pump power of OPO was from 12.5 mW to 28 mW. The experimental results confirm the predicted increase in OPO relaxation frequency with pump power. Squeezing of the single beam intensity was for the first time inferred experimentally by exploiting nature of quantum noise dependent on loss.
Quantum interference of twin optical beams, a typical example of correlated boson fields, is of great interest from the viewpoint of both fundamental and applied physics. Intensity correlated optical beams and their quantum interference bring the possibility of performing sub-shot-noise interferometry experiments which yield high-sensitivity in practical applications. A type-II doubly resonant optical parametric oscillator (OPO) has been built for research in quantum optics, to provide a source of ultrastable quantum correlated (twin) optical beams with continuously tunable frequency difference from zero up to several THz. Three servo loops have been built to control the frequency difference of the twin optical beams and sub-hertz stability has been achieved for frequency difference up to 100MHz. In particular, frequency degenerate twin beams are indistinguishable macroscopic quantum systems. A series of experimental results has been produced with these OPO-generated ultrastable twin beams: the observation of the generalized Hong-Ou-Mandel interference of untrastable twin optical beams, sub-shot-noise homodyne interferometry, and sub-shot-noise heterodyne polarimetry. Note: Abstract extracted from PDF text