Interference pattern formation in the second-order intensity correlation with beams orthogonally polarized

Author(s):  
I. Vidal ◽  
D. P. Caetano ◽  
C. Olindo ◽  
E. J. S. Fonseca ◽  
J. M. Hickmann
2015 ◽  
Vol 32 (12) ◽  
pp. 2431
Author(s):  
Yuchen He ◽  
Jianbin Liu ◽  
Songlin Zhang ◽  
Wentao Wang ◽  
Bin Bai ◽  
...  

2009 ◽  
Vol 07 (01) ◽  
pp. 357-363
Author(s):  
E. WU ◽  
XIAO-AN ZHANG ◽  
XI-MING WANG ◽  
LI-XIA ZENG

We consider a semiconductor quantum well in the excitation system. Applying the pertinent Hamiltonian, we investigate the second-order intensity correlation function and the entanglement properties between the cavity and exciton mode. It is found that nonclassical (antibunching) effect and sudden death effect occur in our system.


Symmetry ◽  
2019 ◽  
Vol 11 (8) ◽  
pp. 1010
Author(s):  
Hyun Geun Lee

We present an efficient linear second-order method for a Swift–Hohenberg (SH) type of a partial differential equation having quadratic-cubic nonlinearity on surfaces to simulate pattern formation on surfaces numerically. The equation is symmetric under a change of sign of the density field if there is no quadratic nonlinearity. We introduce a narrow band neighborhood of a surface and extend the equation on the surface to the narrow band domain. By applying a pseudo-Neumann boundary condition through the closest point, the Laplace–Beltrami operator can be replaced by the standard Laplacian operator. The equation on the narrow band domain is split into one linear and two nonlinear subequations, where the nonlinear subequations are independent of spatial derivatives and thus are ordinary differential equations and have closed-form solutions. Therefore, we only solve the linear subequation on the narrow band domain using the Crank–Nicolson method. Numerical experiments on various surfaces are given verifying the accuracy and efficiency of the proposed method.


2018 ◽  
Vol 59 ◽  
pp. 1-18 ◽  
Author(s):  
Si Hui Pan ◽  
Suruj S. Deka ◽  
Abdelkrim El Amili ◽  
Qing Gu ◽  
Yeshaiahu Fainman

2011 ◽  
Vol 9 (8) ◽  
pp. 081102-81105 ◽  
Author(s):  
曹彬 Bin Cao ◽  
张春熹 Chunxi Zhang ◽  
欧攀 Pan Ou

2018 ◽  
Vol 2018 ◽  
pp. 1-13 ◽  
Author(s):  
M. V. Tinin

The previously obtained integral field representation in the form of double weighted Fourier transform (DWFT) describes effects of inhomogeneities with different scales. The first DWFT approximation describing the first-order effects does not account for incident wave distortions. However, in inhomogeneous media the multiscale second-order effects can also take place when large-scale inhomogeneities distort the field structure of the wave incident on small-scale inhomogeneities. The paper presents the results of the use of DWFT to derive formulas for wave statistical moments with respect to the first- and second-order effects. It is shown that, for narrow-band signals, the second-order effects do not have a significant influence on the frequency correlation. We can neglect the contribution of the second-order effects to the spatial intensity correlation when thickness of the inhomogeneous layer is small, but these effects become noticeable as the layer thickness increases. Accounting for the second-order effects enabled us to get a spatial intensity correlation function, which at large distances goes to the results obtained earlier by the path integral method. This proves that the incident wave distortion effects act on the intensity fluctuations of a wave propagating in a multiscale randomly inhomogeneous medium.


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