A new technique for the study of phase transitions by means of energy dispersive x-ray diffraction. Application to polymeric samples

1996 ◽  
Vol 35 (2) ◽  
pp. 199-213 ◽  
Author(s):  
V. Rossi Albertini ◽  
L. Bencivenni ◽  
R. Caminiti ◽  
F. Cilloco ◽  
C. Sadun
1990 ◽  
Vol 208 ◽  
Author(s):  
E. Chason ◽  
D. T. Warwick

ABSTRACTWe describe a new technique for measuring X-ray reflectivity using energy dispersive X-ray detection. The benefits of this method are the use of a fixed scattering angle and parallel detection of all energies simultaneously. These advantages make the technique more compatible with growth chambers and useable with laboratory X-ray sources. We find excellent agreement between the calculated Fresnel reflectivity and the reflectivity obtained from a smooth Ge (001) surface. Reflectivities obtained during 500 eV Xe ion bombardment of Ge surfaces demonstrate the sensitivity of the technique to be better than 1 Å.


1963 ◽  
Vol 7 ◽  
pp. 209-228 ◽  
Author(s):  
Douglas B. Nash

AbstractResults of an experimental X-ray study on 96 synthetic glasses show that the 2θ positions of glass diffraction maxima have an inverse relation to SiO2 concentration in silicate glasses. This relationship is the basis of a new technique for semiquantitative determinations of SiOa in silicate materials by X-ray diffraction methods. Samples to be examined are fused and the resulting glass scanned from 12 to 40° 2θ using CiiKa radiation. The mean 2θ position of the diffraction maximum is a measure of the SiOs content of the glass. Calibration curves for both weight and molecular percent SiO2 vs. 2θ are presented in this report. The technique requires only small, unweighed amounts of sample for analysis ; it is simple, rapid, and utilizes standard diffraction equipment without modification. Its accuracy, at present, allows SiOa determinations to within ±1 to 4% of the actual concentration.


1992 ◽  
Vol 70 (5) ◽  
pp. 319-321
Author(s):  
G. Leclerc ◽  
J. Beerens ◽  
C. Aktik ◽  
L. Paquin ◽  
M. Isai

We report here a new technique for evaporating polycrystalline InSb films, using hydrogen beams as carriers for each elemental source. The films obtained show X-ray diffraction patterns before annealing that are totally exempt from impurity peaks, unlike those other workers have previously reported for evaporated InSb.


2017 ◽  
Vol 19 (21) ◽  
pp. 14160-14169 ◽  
Author(s):  
Qing Zhang ◽  
Andrea M. Bruck ◽  
David C. Bock ◽  
Jing Li ◽  
Varun Sarbada ◽  
...  

EDXRD was used to profile the phase transitions and spatial phase distribution of a Li1.1V3O8electrode.


1967 ◽  
Vol 6 (12) ◽  
pp. 1393-1396
Author(s):  
Seigô Kishino ◽  
Yoshimitsu Sugita ◽  
Kazutake Kohra

2001 ◽  
Vol 40 (Part 2, No. 7B) ◽  
pp. L718-L720 ◽  
Author(s):  
Kenta Amemiya ◽  
Hiroshi Kondoh ◽  
Akira Nambu ◽  
Masaoki Iwasaki ◽  
Ikuyo Nakai ◽  
...  

MRS Advances ◽  
2017 ◽  
Vol 2 (7) ◽  
pp. 401-406 ◽  
Author(s):  
Qing Zhang ◽  
Andrea M. Bruck ◽  
David C. Bock ◽  
Jing Li ◽  
Eric A. Stach ◽  
...  

ABSTRACTIn this study, we conducted the first energy dispersive x-ray diffraction (EDXRD) experiments on Li/Li1.1V3O8 coin cells discharged to different lithiation levels in order to investigate the phase transitions upon electrochemical reduction. The phase transformation from layered Li-poor α to Li-rich α to defect rock-salt β phase was confirmed with cells of different lithiation stages. No spatial localization of phase formation was observed throughout the cathodes under the conditions of this measurement.


2003 ◽  
Vol 36 (3) ◽  
pp. 920-925 ◽  
Author(s):  
J.-E. Jørgensen ◽  
J. M. Jakobsen ◽  
J. Z. Jiang ◽  
L. Gerward ◽  
J. Staun Olsen

Bulk- and nanocrystalline GaN have been studied by high-pressure energy-dispersive X-ray diffraction. Pressure-induced structural phase transitions from the wurtzite to the NaCl phase were observed in both materials. The transition pressure was found to be 40 GPa for the bulk-crystalline GaN, while the wurtzite phase was retained up to 60 GPa in the case of nanocrystalline GaN. The bulk moduli for the wurtzite phases were determined to be 187 (7) and 319 (10) GPa for the bulk- and nanocrystalline phases, respectively, while the respective NaCl phases were found to have very similar bulk moduli [208 (28) and 206 (44) GPa].


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