Multimode laser model with coupled cavities and quantum noise

1997 ◽  
Vol 14 (1) ◽  
pp. 191 ◽  
Author(s):  
S. E. Hodges ◽  
M. Munroe ◽  
J. Cooper ◽  
M. G. Raymer
1989 ◽  
Vol 40 (5) ◽  
pp. 2410-2416 ◽  
Author(s):  
M. Beck ◽  
I. McMackin ◽  
M. G. Raymer

1988 ◽  
Vol 37 (2) ◽  
pp. 450-455 ◽  
Author(s):  
M. Aguado ◽  
M. San Miguel
Keyword(s):  

1994 ◽  
Vol 50 (5) ◽  
pp. 3453-3457 ◽  
Author(s):  
Pere Colet ◽  
Rajarshi Roy ◽  
Kurt Wiesenfeld
Keyword(s):  

2010 ◽  
Vol 24 (24) ◽  
pp. 4881-4888
Author(s):  
Y. H. LI ◽  
C. S. MA ◽  
D. C. MEI

We study the effects of cross-correlations between the real and imaginary parts of quantum noise on the intensity fluctuation of a saturation laser model. By virtue of the locked phase method,we derived an approximate Fokker–Planck equation and analytic expressions of the stationary probability distribution function (SPD) of the laser system. Based on the SPD, the mean, the normalized variance, and the normalized skewness of the steady-state laser intensity are calculated numerically. The results indicate that the correlation strength of the cross-correlations between the real and imaginary parts of quantum noise increases the intensity fluctuations.


1997 ◽  
Vol 55 (3) ◽  
pp. 2475-2477
Author(s):  
Ya Jia ◽  
Jia-rong Li
Keyword(s):  

Author(s):  
J. Langmore ◽  
M. Isaacson ◽  
J. Wall ◽  
A. V. Crewe

High resolution dark field microscopy is becoming an important tool for the investigation of unstained and specifically stained biological molecules. Of primary consideration to the microscopist is the interpretation of image Intensities and the effects of radiation damage to the specimen. Ignoring inelastic scattering, the image intensity is directly related to the collected elastic scattering cross section, σɳ, which is the product of the total elastic cross section, σ and the eficiency of the microscope system at imaging these electrons, η. The number of potentially bond damaging events resulting from the beam exposure required to reduce the effect of quantum noise in the image to a given level is proportional to 1/η. We wish to compare η in three dark field systems.


Sign in / Sign up

Export Citation Format

Share Document