Optical Mixing with Different Relative Polarization of the Beams

1966 ◽  
Vol 37 (9) ◽  
pp. 3584-3586 ◽  
Author(s):  
H. P. Weber ◽  
E. Mathieu ◽  
K. P. Meyer
1995 ◽  
Vol 78 (11) ◽  
pp. 6477-6480 ◽  
Author(s):  
C. Sammet ◽  
M. Völcker ◽  
W. Krieger ◽  
H. Walther

1998 ◽  
Author(s):  
Mohammed E. Ali ◽  
Daipayan Bhattacharya ◽  
Hernan Erlig ◽  
Harold R. Fetterman ◽  
Mehran Matloubian

2003 ◽  
Vol 67 (12) ◽  
Author(s):  
M. Y. Su ◽  
S. G. Carter ◽  
M. S. Sherwin ◽  
A. Huntington ◽  
L. A. Coldren
Keyword(s):  

1966 ◽  
Vol 19 (8) ◽  
pp. 651-652 ◽  
Author(s):  
M.D. Martin ◽  
E.L. Thomas

2013 ◽  
Vol 22 (01) ◽  
pp. 1350007
Author(s):  
J. L. PAZ ◽  
A. MASTRODOMENICO ◽  
M. A. IZQUIERDO

In this work are studied the symmetry properties of the Rayleigh-type optical mixing signal of a two-level molecular system immersed in a thermal bath and irradiated by a classical electromagnetic field. The solvent induces a random shift of the Bohr frequency in the molecular system. A methodology based in cumulant expansions is employed to obtain the average of the coherences, populations, and susceptibilities of Fourier components associated, calculated by the optical stochastic Bloch equations. These symmetry properties show the dependence of the measured spectra with the variations in the frequencies of the incident fields. Our results show that the inclusion of the thermal bath diminishes the intensity response as well it promotes the loss of the symmetry properties, compared with the same results in the absence of the bath.


2014 ◽  
Vol 613 ◽  
pp. 58-63
Author(s):  
Hai Jin Fu ◽  
Jiu Bin Tan ◽  
Peng Cheng Hu ◽  
Zhi Gang Fan

The heterodyne laser interferometer is widely applied in ultra-precision displacement measurement, but its accuracy is seriously restricted by the optical nonlinearity which arises from the optical mixing in the reference and measurement arms. In an ideal heterodyne laser interferometer, the beam from the laser source consists of two orthogonally linear-polarized components with slightly different optical frequencies and the two components can be completely separated by the polarizing optics, one traverses in the reference arm, the other traverses in the measurement arm, both of them are in the form of a pure optical frequency. However, in a real heterodyne laser interferometer, due to the imperfect laser polarization, the optics defect and the misalignment, the two components of the laser beam cant be perfectly separated, therefore both of the reference arm and the measurement arm contain a portion of the two laser components, which leads to an optical mixing in the two arms of the heterodyne interferometer and causes the cyclic nonlinearity of several to tens of nanometers.


1971 ◽  
Vol 4 (4) ◽  
pp. 300-303 ◽  
Author(s):  
D.C. Hanna ◽  
R.C. Smith ◽  
C.R. Stanley

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