Influence of dysprosium doping on the structural, thermoluminescence and optical properties of lithium aluminium borate

2021 ◽  
Vol 233 ◽  
pp. 117932
Author(s):  
P.O. Ike ◽  
D.E. Folley ◽  
K.K. Agwu ◽  
M.L. Chithambo ◽  
S. Chikwembani ◽  
...  
2022 ◽  
Vol 575 ◽  
pp. 121214
Author(s):  
Osama Bagi Aljewaw ◽  
Muhammad Khalis Abdul Karim ◽  
Halimah Mohamed Kamari ◽  
Mohd Hafiz Mohd Zaid ◽  
Ali Aqeel Salim ◽  
...  

1974 ◽  
Vol 9 (1) ◽  
pp. 63-66 ◽  
Author(s):  
A. A. Filimonov ◽  
N. I. Leonyuk ◽  
L. B. Meissner ◽  
T. I. Timchenko ◽  
I. S. Rez

2012 ◽  
Vol 1020 ◽  
pp. 83-87 ◽  
Author(s):  
Parvinder Kaur ◽  
Gurinder Pal Singh ◽  
Simranpreet Kaur ◽  
D.P. Singh

2020 ◽  
Vol 10 (22) ◽  
pp. 8183
Author(s):  
Osama Bagi Aljewaw ◽  
Muhammad Khalis Abdul Karim ◽  
Halimah Mohamed Kamari ◽  
Mohd Hafiz Mohd Zaid ◽  
Noramaliza Mohd Noor ◽  
...  

In this study, a series of Li2O-Al2O3-B2O3 glasses doped with various concentrations of Dy2O3 (where x = 0.0, 0.2, 0.4, 0.6, 0.8, and 1.0 mol%) were prepared by using a conventional melt-quenching technique. The structural, physical and optical properties of the glasses were examined by utilising a variety of techniques instance, X-ray diffraction (XRD), UV–Vis-NIR spectrometer, Fourier transform infrared (FTIR) and photoluminescence (PL). The XRD spectra demonstrate the amorphous phase of all glasses. Furthermore, the UV-vis-NIR spectrometers have registered optical absorption spectra a numbers of peaks which exist at 1703, 1271, 1095, 902, 841, 802, 669, 458, 393 and 352 nm congruous to the transitions from the ground of state (6H15/2) to different excited states, 6H11/2, 6F11/2 + 6H9/2, 6F9/2 + 6H7/2, 6F7/2, 6F5/2, 6F3/2, 4F9/2, 4I15/2, 4F7/2 and 6P7/2, respectively. The spectra of emission exhibit two strong emanation bands at 481 nm and 575 nm in the visible region, which correspond to the transitions 4F9/2 → 6H15/2 and 4F9/2 → 6H13/2. All prepared glass samples doped with Dy2O3 show an increase in the emission intensity with an increase in the concentration of Dy3+. Based on the obtained results, the aforementioned glass samples may have possible applications, such as optical sensor and laser applications.


1997 ◽  
Vol 51 ◽  
pp. 1045-1050 ◽  
Author(s):  
Johan Åhman ◽  
Göran Svensson ◽  
Jekabs Grins ◽  
Jose M. Dominguez-Vera ◽  
Jose Maria Moreno ◽  
...  

2004 ◽  
Vol 16 (3) ◽  
pp. 465-471 ◽  
Author(s):  
R Martínez Vázquez ◽  
R Osellame ◽  
M Marangoni ◽  
R Ramponi ◽  
E Diéguez ◽  
...  

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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