RP Photonics logo
VL logo part of the
Virtual
Library

Encyclopedia of Laser Physics and Technology

Squeezed States of Light

previous  |  next  |  feedback

Definition: nonclassical states of light with noise below the standard quantum limit in one quadrature component

Squeezed states of light (or squeezed light) are a kind of nonclassical light and constitute an interesting subject of quantum optics, the experimental investigation of which began in the 1980s.

Squeezed light is best understood by considering complex phasors for the representation of the state of light in one mode of the optical field. Classically, such a state can be represented by a certain phasor (or its end point in the complex plane). According to quantum optics, however, there is a quantum uncertainty, and any measurement of the complex amplitude of the light field can deliver different values within an uncertainty region. Moreover, there is an uncertainty relation for the quadrature components of the light field, saying that the product of the uncertainties in both components is at least some quantity times Planck's constant.

Glauber's coherent states have circularly symmetric uncertainty regions, so that the uncertainty relation dictates some minimum noise amplitudes e.g. for the amplitude and phase. A further reduction in, e.g., amplitude noise is possible only by “squeezing” the uncertainty region, reducing its width in the amplitude direction while increasing it in the orthogonal direction, so that the phase uncertainty is increased. Such light is called amplitude-squeezed (see Figure 1, left). Conversely, phase-squeezed light (Figure 1, middle) has decreased phase fluctuations at the expense of increased amplitude fluctuations.

squeezed states of light

Figure 1: Different squeezed states of light, illustrated in phasor diagrams. The blue ellipses indicate the uncertainty regions.

Of course, there are also squeezed states where the orientation of the uncertainty region is different from the cases shown, or where the shape of the uncertainty region is different from that of an ellipse. In any case, some noise component is below the standard quantum limit.

There is also the so-called squeezed vacuum (Figure 1, right), where the center of the uncertainty region (corresponding to the average amplitude) is at the origin of the coordinate system, and the fluctuations are reduced in some direction. The mean photon number is larger than zero in this case; a squeezed vacuum is a “vacuum” only in the sense that the average amplitude (but not the average photon number) is zero. Squeezed light with a non-zero average amplitude is also called bright squeezed light.

Quantum noise also leads to fluctuations of the polarization, which are reduced in polarization-squeezed light.

Generation of Squeezed Light

Squeezed light can be generated from light in a coherent state or vacuum state by using certain optical nonlinear interactions. For example, an optical parametric amplifier with a vacuum input can generate a squeezed vacuum with a reduction in the noise of one quadrature components by the order of 10 dB. A lower degree of squeezing in bright amplitude-squeezed light can under some circumstances be obtained with frequency doubling. The Kerr nonlinearity in optical fibers also allows the generation of amplitude-squeezed light. Semiconductor lasers can generate amplitude-squeezed light when operated with a carefully stabilized pump current. Squeezing can also arise from atom-light interactions.

Applications

In principle, squeezed light can be used in a number of areas, as it allows for measurements with reduced quantum noise. An example is the ultraprecise measurement of lengths for the detection of gravitational waves with large-scale interferometers. However, the use of squeezed light is not very widespread, basically because it is plagued with various difficulties. For example, any optical losses bring a squeezed state of light closer to a coherent state, i.e. tend to destroy the nonclassical properties. At least in fundamental quantum optics research, however, squeezed states of light play an important role.

Bibliography

[1]C. M. Caves, “Quantum limits on noise in linear amplifiers”, Phys. Rev. D 26 (8), 1817 (1982)
[2]D. Walls, “Squeezed states of light”, Nature 306, 141 (1983)
[3]R. E. Slusher et al., “Observation of squeezed states generated by four wave mixing in an optical cavity”, Phys. Rev. Lett. 55 (22), 2409 (1985)
[4]S. Machida et al., “Observation of amplitude squeezing in a constant-current-driven semiconductor laser”, Phys. Rev. Lett. 58 (10), 1000 (1987)
[5]P. Grangier et al., “Squeezed light-enhanced polarization interferometer”, Phys. Rev. Lett. 59 (19), 2153 (1987)
[6]H. J. Kimble and D. Walls (eds.), special issue on squeezed light in J. Opt. Soc. Am B 4 (10) (1987)
[7]R. E. Slusher et al., “Pulsed squeezed light”, Phys. Rev. Lett. 59 (22), 2566 (1987)
[8]S. F. Pereira et al., “Generation of squeezed light by intracavity frequency doubling”, Phys. Rev. A 38 (9), 4931 (1988)
[9]W. H. Richardson et al., “Squeezed photon-number noise and sub-Poissonian electrical partition noise in a semiconductor laser”, Phys. Rev. Lett. 66 (22), 2867 (1991)
[10]E. S. Polzik et al., “Spectroscopy with squeezed light”, Phys. Rev. Lett. 68 (20), 3020 (1992)
[11]R. Paschotta et al., “Bright squeezed light from a singly-resonant frequency doubler”, Phys. Rev. Lett. 72 (24), 3807 (1994)
[12]G. Breitenbach et al., “Squeezed vacuum from a monolithic optical parametric oscillator”, J. Opt. Soc. Am. B 12 (11), 2304 (1995)
[13]S. Schmitt et al., “Photon-number squeezed solitons from an asymmetric fiber-optic Sagnac interferometer”, Phys. Rev. Lett. 81 (12), 2446 (1998)
[14]M. Margalit et al., “Cross phase modulation squeezing in optical fibers”, Opt. Express 2 (3), 72 (1998)
[15]Y. Takeno et al., “Observation of −9 dB quadrature squeezing with improvement of phase stability in homodyne measurement”, Opt. Express 15 (7), 4321 (2007)
[16]H. Vahlbruch et al., “Observation of squeezed light with 10 dB quantum noise reduction”, Phys. Rev. Lett. 100, 033602 (2008)

See also: quantum optics, coherent states, intensity noise, phase noise, amplitude-squeezed light, nonclassical light, standard quantum limit

Categories: fluctuations and noise, quantum optics

arrow
Home New articles Spotlight Feedback Advertising
Categories Search Quiz Links Page hits
S

This encyclopedia is provided by
RP Photonics Consulting GmbH.

Utilize the expertise of the author, Dr. Rüdiger Paschotta, also in the form of technical consulting services!

RP Q-switch

A powerful software tool for designing
Q-switched lasers. See the details.

Onefive logo

Onefive

Low-noise
femtosecond,
picosecond,
and tunable single-frequency lasers for OEM and R&D applications.

A.L.S. logo

A.L.S. GmbH

Picosecond laser diodes
<30 ps, 375 – 1600 nm, >1 Wp, single shot – 120 MHz

RP Fiber Power

This software helps to design and analyze fiber amplifiers and lasers.

Field Guide to Lasers

This new book by Dr. Paschotta explains principles and types of lasers.

TRUMPF logo

TRUMPF-Laser

a leading supplier of industrial diode pumped solid state lasers,
CO2 lasers, and laser systems for material processing.

Your Advertisement at This Place

will be seen by many thousands of visitors per month. These banners receive far over 100'000 page hits per month. Check the details.