X-ray polarimetry and position measurements using the photoeffect and diffusion in a CCD

Author(s):  
Klaus H. Schmidt ◽  
Gerd W. Buschhorn ◽  
Rainer Kotthaus ◽  
Matthias Rzepka ◽  
Peter M. Weinmann
Keyword(s):  
X Ray ◽  
Title X ◽  
2009 ◽  
Vol 610-613 ◽  
pp. 1150-1154
Author(s):  
Ai Lan Fan ◽  
Cheng Gang Zhi ◽  
Lin Hai Tian ◽  
Lin Qin ◽  
Bin Tang

The Mo surface modified layer on Ti6Al4V alloy was obtained by the plasma surface alloying technique. The structure and composition of the Mo modified Ti6Al4V alloy was investigated by X-ray diffraction (XRD) and glow discharge optical emission spectroscopy (GDOES). The Mo modified layer contains Mo coating on subsurface and diffusion layers between the subsurface and substrate. The X- ray diffraction analysis of the Mo modified Ti6Al4V alloy reveals that the outmost surface of the Mo modified Ti6Al4V alloy is composed of pure Mo. The electrochemical corrosion performance of the Mo modified Ti6Al4V alloy in 25°C Hank’s solution was investigated and compared with that of Ti6Al4V alloy. Results indicate that the self-corroding electric potential and the corrosion-rate of the Mo modified Ti6Al4V alloy are higher than that of Ti6Al4V alloy in 25°C Hank’s solution.


1984 ◽  
Author(s):  
B Fay ◽  
W T. Novak
Keyword(s):  
X Ray ◽  
Title X ◽  

1998 ◽  
Author(s):  
Masaki Koike ◽  
Isao H. Suzuki ◽  
Satoshi Komiya
Keyword(s):  
X Ray ◽  

1997 ◽  
Author(s):  
Henryk Fiedorowicz
Keyword(s):  
X Ray ◽  

1996 ◽  
Author(s):  
Sabee Y. Molloi ◽  
Jerry Tang ◽  
Martin R. Marcin ◽  
Yifang Zhou ◽  
Behzad Anvar
Keyword(s):  
X Ray ◽  

1998 ◽  
Author(s):  
Yoshiki Kohmura ◽  
Mitsuhiro Awaji ◽  
Yoshio Suzuki ◽  
Tetsuya Ishikawa
Keyword(s):  
X Ray ◽  
Title X ◽  

Minerals ◽  
2021 ◽  
Vol 11 (3) ◽  
pp. 325
Author(s):  
Sytle Antao

Synchrotron high-resolution powder X-ray diffraction (HRPXRD) and Rietveld structure refinements were used to examine the crystal structure of single phases and intergrowths (either two or three phases) in 13 samples of the helvine-group minerals, (Zn,Fe,Mn)8[Be6Si6O24]S2. The helvine structure was refined in the cubic space group P4¯3n. For the intergrowths, simultaneous refinements were carried out for each phase. The structural parameters for each phase in an intergrowth are only slightly different from each other. Each phase in an intergrowth has well-defined unit-cell and structural parameters that are significantly different from the three endmembers and these do not represent exsolution or immiscibility gaps in the ternary solid-solution series. The reason for the intergrowths in the helvine-group minerals is not clear considering the similar radii, identical charge, and diffusion among the interstitial M cations (Zn2+, Fe2+, and Mn2+) that are characteristic of elongated tetrahedral coordination. The difference between the radii of Zn2+ and Mn2+ cations is 10%. Depending on the availability of the M cations, intergrowths may occur as the temperature, pressure, fugacity fS2, and fluid composition change on crystallization. The Be–Si atoms are fully ordered. The Be–O and Si–O distances are nearly constant. Several structural parameters (Be–O–Si bridging angle, M–O, M–S, average <M–O/S>[4] distances, and TO4 rotational angles) vary linearly with the a unit-cell parameter across the series because of the size of the M cation.


1994 ◽  
Author(s):  
Kunio Shinohara ◽  
Atsushi Ito ◽  
Yasuhito Kinjo
Keyword(s):  
X Rays ◽  
X Ray ◽  

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