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Squeezed light

For a light source of a specific power, there is a fundamental limit to the precision to which the intensity can be determined within a specific period. This is termed the shot-noise limit. If n photons are accumulated, the variance is /n and the signal-to-noise ratio (S/N) is fnln. Any additional noise source (due to the amphfier, interference or detector imperfections) will degrade this value. Theoretically, shot-noise in coherently squeezed light can be slightly lower than this limit, but ultimately only by a factor of 1/ 2. [Pg.6523]

Let us now turn to squeezed light. We define quadrature components of single and compound modes ... [Pg.562]

Because of the linearity of Heisenberg-Langevin equations, the squeezing does not depend on the initial complex amplitudes of optical modes. Squeezed light... [Pg.562]

Popp FA, Chang JJ, Herzog A, Yan Z, Yan Y. Evidence of non-classical (squeezed) light in biological systems. Phys Lett A 2002 293 98-102. [Pg.66]

Squeezing Light Near-field Scanning Optical Microscopy... [Pg.1213]

Another example, where a beam of squeezed light was realized with 3.2 mW and 52 % noise reduction, is the second-harmonic generation with a cw Nd YAG laser in a monolithic resonator [1337]. The experimental setup is shown in Fig. 9.101a. [Pg.583]

Fig. 9.101 (a) Experimental setup for the generation of bright squeezed light by second-harmonic generation in a monolithic resonator (b) spectral power density of photocurrent fluctuations for squeezed light input to a balanced homodyne detector. The upper curve (/> gives the shot-noise level [1337]... [Pg.584]

In Sect. 9.8.1 it was shown that the noise limit without squeezing is caused by the zero-point field coupled into the second input part of the interferometer. If a beam of squeezed light is fed into this input part, the noise level can be decreased and the detectable length change AL can be further decreased [1356]. [Pg.586]

The combination of Ramsey spectroscopy (see Sect. 9.3) and squeezed light has brought an increased spectral resolution. While traditional Ramsey spectroscopy allows the resolution Am = 2nl2>T where T is the flight time of the molecules between the two separated fields, using two-mode squeezed light and two-atom excitation with joint detection a spectral resolution oin/3T could be achieved [1355]. [Pg.586]

P. Kurz, R. Paschotta, K. Fiedler, J. Mlynek, Bright squeezed light by second harmonic generation and monolytic resonator. Europhys. Lett. 24,449 (1993)... [Pg.738]

K. Qu, G.S. Agaral, Ramsey spectroscopy using squeezed light. Opt. Lett. 38,2563 (2013)... [Pg.739]

J. Bergou, C. Benkert, L. Davidovich and et al. Double two-photon correlated-spontaneous-emission lasers as bright sources of squeezed light. Physical Revew A 1990 Nov l 42(9) 5544-5552. [Pg.94]

Klaus M. Gheri, Daniel F. Walls. Lossless transformation of coherent light into amplitude-squeezed light. Physical Revew A 1992 Dec 1 46(11) R6793 - R6796. [Pg.96]

T. C. Ralph, C. M. Savage. Squeezed light from a coherently pumped four-level laser Physical Revew A 1991 Dec 1 44(11) 7809-7814. [Pg.96]

Appel J, Figueroa E, Korystov D et al. Quantum memory for squeezed light. Physical Review Letters 2008 Mar 5 100(9) 093602(4). [Pg.126]

Fluid coking—a process that uses a reactor to scrape the bottom of the barrel and squeeze light products out of the residue. [Pg.248]


See other pages where Squeezed light is mentioned: [Pg.329]    [Pg.3]    [Pg.62]    [Pg.125]    [Pg.61]    [Pg.493]    [Pg.494]    [Pg.556]    [Pg.563]    [Pg.565]    [Pg.739]    [Pg.14]    [Pg.420]    [Pg.355]    [Pg.50]    [Pg.51]    [Pg.480]    [Pg.160]    [Pg.167]    [Pg.168]   
See also in sourсe #XX -- [ Pg.3 ]




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