Dispersion characteristics of nanometer-scaled silicon rib waveguides

2010 ◽  
Vol 8 (5) ◽  
pp. 485-489 ◽  
Author(s):  
贾连希 Lianxi Jia ◽  
耿敏明 Minming Geng ◽  
张磊 Lei Zhang ◽  
杨林 Lin Yang ◽  
陈平 Ping Chen ◽  
...  
2015 ◽  
Vol 350 ◽  
pp. 241-247 ◽  
Author(s):  
Jinkun Liao ◽  
Xiongui Tang ◽  
Yuan Gao ◽  
Wenjie Wan ◽  
Xiaoxia Zhang ◽  
...  

2015 ◽  
Vol 36 (5) ◽  
pp. 526-533
Author(s):  
廖进昆 LIAO Jin-kun ◽  
唐雄贵 TANG Xiong-gui ◽  
高原 GAO yuan ◽  
万文杰 WAN Wen-jie ◽  
张晓霞 ZHANG Xiao-xia ◽  
...  

2013 ◽  
Vol 33 (5) ◽  
pp. 0513001
Author(s):  
刘珊 Liu Shan ◽  
沈祥 Shen Xiang ◽  
徐铁峰 Xu Tiefeng ◽  
陈昱 Chen Yu ◽  
陈芬 Chen Fen ◽  
...  

1988 ◽  
Vol 102 ◽  
pp. 79-81
Author(s):  
A. Goldberg ◽  
S.D. Bloom

AbstractClosed expressions for the first, second, and (in some cases) the third moment of atomic transition arrays now exist. Recently a method has been developed for getting to very high moments (up to the 12th and beyond) in cases where a “collective” state-vector (i.e. a state-vector containing the entire electric dipole strength) can be created from each eigenstate in the parent configuration. Both of these approaches give exact results. Herein we describe astatistical(or Monte Carlo) approach which requires onlyonerepresentative state-vector |RV> for the entire parent manifold to get estimates of transition moments of high order. The representation is achieved through the random amplitudes associated with each basis vector making up |RV>. This also gives rise to the dispersion characterizing the method, which has been applied to a system (in the M shell) with≈250,000 lines where we have calculated up to the 5th moment. It turns out that the dispersion in the moments decreases with the size of the manifold, making its application to very big systems statistically advantageous. A discussion of the method and these dispersion characteristics will be presented.


1990 ◽  
Vol 137 (1) ◽  
pp. 21 ◽  
Author(s):  
M.S. Stern ◽  
P.C. Kendall ◽  
P.W.A. McLlroy

1997 ◽  
Vol 51 (8) ◽  
pp. 77-84
Author(s):  
L. M. Buzik ◽  
O. F. Pishko ◽  
S.A. Churilova ◽  
O. I. Sheremet

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