Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure

Phase stability of various phases of MX (M=Ti, Zr; X=C, N) at equilibrium and under pressure is examined based on first-principles calculations of the electronic and phonon structures. The results reveal that all B1 (NaCl-type) MX structures undergo a phase transition to the B2-structures under high...

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Main Authors: V.I. Ivashchenko, P.E.A. Turchi, V.I. Shevchenko
Format: Article
Language:English
Published: Institute for Condensed Matter Physics 2013-01-01
Series:Condensed Matter Physics
Subjects:
Online Access:http://dx.doi.org/10.5488/CMP.16.33602
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author V.I. Ivashchenko
P.E.A. Turchi
V.I. Shevchenko
author_facet V.I. Ivashchenko
P.E.A. Turchi
V.I. Shevchenko
author_sort V.I. Ivashchenko
collection DOAJ
description Phase stability of various phases of MX (M=Ti, Zr; X=C, N) at equilibrium and under pressure is examined based on first-principles calculations of the electronic and phonon structures. The results reveal that all B1 (NaCl-type) MX structures undergo a phase transition to the B2-structures under high pressure in agreement with the previous total-energy calculations. The B1-MX structures are dynamically stable under very high pressure (210-570 GPa). The pressure-induced B2 (CsCl-type) MC phases are dynamically unstable even at high pressures, and TiN and ZrN are found to crystallize with the B2-structure only at pressures above 55 GPa. The first-order B1-to-B2 phase transition in these nitrides is not related to the softening of phonon modes, and the dynamical instability of B2-MX is associated with a high density of states at the Fermi level.
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spelling doaj.art-eec9ff78c786411cb021fb1e8ce50a2a2022-12-22T01:32:16ZengInstitute for Condensed Matter PhysicsCondensed Matter Physics1607-324X2013-01-011633360210.5488/CMP.16.33602Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressureV.I. IvashchenkoP.E.A. TurchiV.I. ShevchenkoPhase stability of various phases of MX (M=Ti, Zr; X=C, N) at equilibrium and under pressure is examined based on first-principles calculations of the electronic and phonon structures. The results reveal that all B1 (NaCl-type) MX structures undergo a phase transition to the B2-structures under high pressure in agreement with the previous total-energy calculations. The B1-MX structures are dynamically stable under very high pressure (210-570 GPa). The pressure-induced B2 (CsCl-type) MC phases are dynamically unstable even at high pressures, and TiN and ZrN are found to crystallize with the B2-structure only at pressures above 55 GPa. The first-order B1-to-B2 phase transition in these nitrides is not related to the softening of phonon modes, and the dynamical instability of B2-MX is associated with a high density of states at the Fermi level.http://dx.doi.org/10.5488/CMP.16.33602titanium and zirconium carbides and nitridesfirst-principles calculationsphase transformationelectronic and phonon structures
spellingShingle V.I. Ivashchenko
P.E.A. Turchi
V.I. Shevchenko
Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure
Condensed Matter Physics
titanium and zirconium carbides and nitrides
first-principles calculations
phase transformation
electronic and phonon structures
title Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure
title_full Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure
title_fullStr Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure
title_full_unstemmed Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure
title_short Phase transformation B1 to B2 in TiC, TiN, ZrC and ZrN under pressure
title_sort phase transformation b1 to b2 in tic tin zrc and zrn under pressure
topic titanium and zirconium carbides and nitrides
first-principles calculations
phase transformation
electronic and phonon structures
url http://dx.doi.org/10.5488/CMP.16.33602
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AT peaturchi phasetransformationb1tob2intictinzrcandzrnunderpressure
AT vishevchenko phasetransformationb1tob2intictinzrcandzrnunderpressure