Perfluoropolymer Optical Waveguide Comparable to Silica in Optical Properties and Reliabilities

Author(s):  
Yasuhiro Kuwana ◽  
Kousuke Takayama ◽  
Shotaro Takenobu ◽  
Yoshitomi Morizawa
2014 ◽  
Vol 2 (6) ◽  
pp. 1004-1009 ◽  
Author(s):  
Yang Liu ◽  
Xin Ye ◽  
Guangfeng Liu ◽  
Yun Lv ◽  
Xiying Zhang ◽  
...  

The aggregation-induced emission (AIE) characteristics a carbazole-containing alkene enable its highly blue emissive crystal fibers exhibit optical waveguide effect.


2020 ◽  
Vol 459 ◽  
pp. 124945
Author(s):  
Haodong Zhu ◽  
Xiangbo Yang ◽  
Zebiao Lin ◽  
Xianhong Liu ◽  
Xinyu Yang

1992 ◽  
Vol 247 ◽  
Author(s):  
Patrick G. Jobe ◽  
Christine Puglisi ◽  
Z. X. Zhu ◽  
K. J. Fang ◽  
D. Liu ◽  
...  

THERMID, made of acetylene-terminated polyimide oligomers, was developed by National Starch & Chemical Co. It is capable of forming thicker deposits than conventional polyimides. It is a candidate for a broad array of electronic and optoelectronic applications, including passivation coating, alpha-particle barrier, interlayer dielectric, encapsulation of discrete devices and IC, optical waveguide, and multilayer dielectric for thin hybrids. The study and evaluation of electrical and optical properties of THERMID polyimide give more support to their application in the semiconductor industry.


2011 ◽  
Author(s):  
J. M. Gutiérrez ◽  
S. Camacho-López ◽  
M. Cano-Lara ◽  
A. Rodríguez ◽  
R. E. Balderas-Navarro ◽  
...  

Author(s):  
K. Tsuno ◽  
T. Honda ◽  
Y. Harada ◽  
M. Naruse

Developement of computer technology provides much improvements on electron microscopy, such as simulation of images, reconstruction of images and automatic controll of microscopes (auto-focussing and auto-correction of astigmatism) and design of electron microscope lenses by using a finite element method (FEM). In this investigation, procedures for simulating the optical properties of objective lenses of HREM and the characteristics of the new lens for HREM at 200 kV are described.The process for designing the objective lens is divided into three stages. Stage 1 is the process for estimating the optical properties of the lens. Firstly, calculation by FEM is made for simulating the axial magnetic field distributions Bzc of the lens. Secondly, electron ray trajectory is numerically calculated by using Bzc. And lastly, using Bzc and ray trajectory, spherical and chromatic aberration coefficients Cs and Cc are numerically calculated. Above calculations are repeated by changing the shape of lens until! to find an optimum aberration coefficients.


Author(s):  
A. Strojnik ◽  
J.W. Scholl ◽  
V. Bevc

The electron accelerator, as inserted between the electron source (injector) and the imaging column of the HVEM, is usually a strong lens and should be optimized in order to ensure high brightness over a wide range of accelerating voltages and illuminating conditions. This is especially true in the case of the STEM where the brightness directly determines the highest resolution attainable. In the past, the optical behavior of accelerators was usually determined for a particular configuration. During the development of the accelerator for the Arizona 1 MEV STEM, systematic investigation was made of the major optical properties for a variety of electrode configurations, number of stages N, accelerating voltages, 1 and 10 MEV, and a range of injection voltages ϕ0 = 1, 3, 10, 30, 100, 300 kV).


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