Correction and Addendum to the Paper "The Optical Properties of Hydrochloric-Boric Acid Mixtures"1

1962 ◽  
Vol 32 (1_2) ◽  
pp. 127-131 ◽  
Author(s):  
Kurze Mitteilung
1984 ◽  
Vol 31-32 ◽  
pp. 789-791 ◽  
Author(s):  
Mark A. Kramer ◽  
Wayne R. Tompkin ◽  
Jerzy Krasinski ◽  
Robert W. Boyd

1990 ◽  
Vol 29 (27) ◽  
pp. 3921 ◽  
Author(s):  
Wayne R. Tompkin ◽  
Michelle S. Malcuit ◽  
Robert W. Boyd

1959 ◽  
Vol 19 (3_4) ◽  
pp. 193-201 ◽  
Author(s):  
Hussein Sadek ◽  
Th. F. Tadros

2021 ◽  
Author(s):  
Yi Cheng ◽  
Wenwen Fan ◽  
Longjie Wang ◽  
Yanxiong Liu ◽  
Qiufeng Wang ◽  
...  

Abstract Ultralong room-temperature phosphorescence (URTP) materials with photo stimulus responsive (named URTP-PSR) behavior are amazing but still rarely reported due to their great requirements on the crystal structure, complicated synthesis process, long photo-activation and deactivation time. Herein, a series of URTP-PSR materials were prepared by a facile doping process, which involved one-pot heating treatment of benzoic acid derivatives and boric acid to form an amorphous phase. The URTP-PSR materials displayed gradually enhanced ultra-long phosphorescence upon prolonged deep UV light illumination under ambient conditions to restricts the vibration and rotation of molecular. Impressively, both of the photo-activation and deactivation process can be finished within several seconds, which was much fast than previously reported URTP-PSR materials. The optical properties can be repeated many times without obvious loosing performance, suggesting excellent fatigue resistance behaviors of the URTP-PSR materials. Simultaneously, the URTP-PSR materials also displayed excellent atmosphere stability, which still maintained good optical properties even under oxygen atmosphere. Furthermore, owing to the high processability and light-stimulus emission, the URTP-PSR materials have been utilized as security ink for anti-counterfeiting pattern application. It's worth mentioning that all the raw materials are commercialized and low-cost, which could be purchased directly and benefit for the practical application. These findings break through many limitations of existing dynamic RTP materials, such as complicated preparation process, fine crystal structure, long photo-activation and deactivation time, and furthermore expand the scope of dynamic smart-response materials for great potential in many fields.


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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