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Compression of Ti 3 Si 0.5 Ge 0.5 C 2 to 53 GPa

Using a synchrotron radiation source and a diamond anvil cell, we measured the pressure dependence of the lattice parameters of a polycrystalline Ti 3 Si 0.5 Ge 0.5 C 2 sample. Up to a pressure of 53 GPa, no phase transformations were observed. As for the isostructural hexagonal Ti 3 SiC 2 , the com... Full description

Journal Title: Applied Physics Letters 12 April 2004, Vol.84(15), pp.2799-2801
Main Author: Manoun, Bouchaib
Other Authors: Liermann, H. P. , Gulve, R. P. , Saxena, S. K. , Ganguly, A. , Barsoum, M. W. , Zha, C. S.
Format: Electronic Article Electronic Article
Language: English
Subjects:
Quelle: © 2004 American Institute of Physics (AIP)
ID: ISSN: 0003-6951 ; E-ISSN: 1077-3118 ; DOI: 10.1063/1.1699477
Link: http://dx.doi.org/10.1063/1.1699477
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recordid: aip_complete10.1063/1.1699477
title: Compression of Ti 3 Si 0.5 Ge 0.5 C 2 to 53 GPa
format: Article
creator:
  • Manoun, Bouchaib
  • Liermann, H. P.
  • Gulve, R. P.
  • Saxena, S. K.
  • Ganguly, A.
  • Barsoum, M. W.
  • Zha, C. S.
subjects:
  • Structural, Mechanical, Thermodynamic, And Optical Properties Of Condensed Matter
ispartof: Applied Physics Letters, 12 April 2004, Vol.84(15), pp.2799-2801
description: Using a synchrotron radiation source and a diamond anvil cell, we measured the pressure dependence of the lattice parameters of a polycrystalline Ti 3 Si 0.5 Ge 0.5 C 2 sample. Up to a pressure of 53 GPa, no phase transformations were observed. As for the isostructural hexagonal Ti 3 SiC 2 , the compressibility along the c axis was greater than along a . The bulk modulus is 183±4  GPa with a pressure derivative of 3.4±0.2. This work shows that the replacement of Si by Ge in Ti 3 SiC 2 results in a systematic decrease in the bulk moduli.
language: eng
source: © 2004 American Institute of Physics (AIP)
identifier: ISSN: 0003-6951 ; E-ISSN: 1077-3118 ; DOI: 10.1063/1.1699477
fulltext: fulltext
issn:
  • 0003-6951
  • 1077-3118
  • 00036951
  • 10773118
url: Link


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titleCompression of Ti 3 Si 0.5 Ge 0.5 C 2 to 53 GPa
creatorManoun, Bouchaib ; Liermann, H. P. ; Gulve, R. P. ; Saxena, S. K. ; Ganguly, A. ; Barsoum, M. W. ; Zha, C. S.
ispartofApplied Physics Letters, 12 April 2004, Vol.84(15), pp.2799-2801
subjectStructural, Mechanical, Thermodynamic, And Optical Properties Of Condensed Matter
descriptionUsing a synchrotron radiation source and a diamond anvil cell, we measured the pressure dependence of the lattice parameters of a polycrystalline Ti 3 Si 0.5 Ge 0.5 C 2 sample. Up to a pressure of 53 GPa, no phase transformations were observed. As for the isostructural hexagonal Ti 3 SiC 2 , the compressibility along the c axis was greater than along a . The bulk modulus is 183±4  GPa with a pressure derivative of 3.4±0.2. This work shows that the replacement of Si by Ge in Ti 3 SiC 2 results in a systematic decrease in the bulk moduli.
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descriptionUsing a synchrotron radiation source and a diamond anvil cell, we measured the pressure dependence of the lattice parameters of a polycrystalline Ti 3 Si 0.5 Ge 0.5 C 2 sample. Up to a pressure of 53 GPa, no phase transformations were observed. As for the isostructural hexagonal Ti 3 SiC 2 , the compressibility along the c axis was greater than along a . The bulk modulus is 183±4  GPa with a pressure derivative of 3.4±0.2. This work shows that the replacement of Si by Ge in Ti 3 SiC 2 results in a systematic decrease in the bulk moduli.
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abstractUsing a synchrotron radiation source and a diamond anvil cell, we measured the pressure dependence of the lattice parameters of a polycrystalline Ti 3 Si 0.5 Ge 0.5 C 2 sample. Up to a pressure of 53 GPa, no phase transformations were observed. As for the isostructural hexagonal Ti 3 SiC 2 , the compressibility along the c axis was greater than along a . The bulk modulus is 183±4  GPa with a pressure derivative of 3.4±0.2. This work shows that the replacement of Si by Ge in Ti 3 SiC 2 results in a systematic decrease in the bulk moduli.
pubAmerican Institute of Physics
doi10.1063/1.1699477
date2004-04-12