New approach for obtaining the time-evolution law of a chaotic light field in a damping—gaining process

2012 ◽  
Vol 21 (8) ◽  
pp. 080302 ◽  
Author(s):  
Li-Hua Gong ◽  
Nan-Run Zhou ◽  
Li-Yun Hu ◽  
Hong-Yi Fan
1997 ◽  
Vol 04 (05) ◽  
pp. 901-905
Author(s):  
J. B. PENDRY

Low energy electron diffraction experiments have superb sensitivity to surface structure, but rely on sophisticated theory for their interpretation. Advances in computer power, and developments in the theory itself, enable us to handle surface structures of moderate complexity. For future advances we must look to a completely new approach and the case is made for order-N methods which follow the time evolution of a point source of electrons to generate all beams for all angles of incidence and all energies in one shot.


2011 ◽  
Vol 20 (02) ◽  
pp. 155-165 ◽  
Author(s):  
K. V. PRIYESH ◽  
RAMESH BABU THAYYULLATHIL

We have investigated the interaction of two level atom with time varying quadrature squeezed light field. Jaynes-Cummings model is used for solving the atom radiation interaction. Time evolution of the system for different squeezing parameter and phase have been studied. There are no well-defined revivals in population inversion when the squeezed phase is π and the squeezing parameter is greater than 0.5. Using a time varying frequency for the light field, it is found that the randomness of the population inversion and the collapse revival phenomena can be controlled. Frequency modulation of the field can thus be used as a tool for manipulating the squeezed light atom interaction.


2015 ◽  
Vol 93 (3) ◽  
pp. 283-289 ◽  
Author(s):  
Cheng Da ◽  
Qian-Fan Chen ◽  
Peng-Fei Zhang ◽  
Hong-Yi Fan

We examine how a Laguerre-polynomial-weighted chaotic photon field (LPWCPF), whose density operator is [Formula: see text], evolves in an amplitude-damping channel. By using a newly derived generating function of two-variable Hermite polynomials we obtain the evolution law of LPWCPF, which turns out to be a new LPWCPF with a new parameter, depending on 1 − e−2κt, where κ represents decay rate. The technique of integration (summation) within an ordered product of operators is used in our discussions.


2010 ◽  
Vol 37 (2) ◽  
pp. 135-136 ◽  
Author(s):  
Jovan K. Popović ◽  
Milica T. Atanacković ◽  
Ana S. Pilipović ◽  
Milan R. Rapaić ◽  
Stevan Pilipović ◽  
...  

2010 ◽  
Vol 38 (1) ◽  
pp. 163-164
Author(s):  
Jovan K. Popović ◽  
Milica T. Atanacković ◽  
Ana S. Pilipović ◽  
Milan R. Rapaić ◽  
Stevan Pilipović ◽  
...  

2010 ◽  
Vol 37 (2) ◽  
pp. 119-134 ◽  
Author(s):  
Jovan K. Popović ◽  
Milica T. Atanacković ◽  
Ana S. Pilipović ◽  
Milan R. Rapaić ◽  
Stevan Pilipović ◽  
...  

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