2022
DOI: 10.1021/acs.jpcc.2c02416
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High-Pressure Structural Transformation Pathway and Electronic Properties of AgGaTe2: Ab Initio Evolutionary Structural Searching

Abstract: We have used systematic ab initio evolutionary structural searching to uncover the high-pressure transformation pathway of a promising thermoelectric material, AgGaTe2. The global structures of the ternary Ag–Ga–Te system have been predicted up to 100 GPa. The known chalcopyrite phase at ambient pressure is validated by the searching method. The B3-like structure with the space group (s.g.) of P4̅m 2 exhibits a metastable one at a low-pressure range. The first structural phase transition is calculated at about… Show more

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Cited by 4 publications
(3 citation statements)
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“…When materials undergo high pressure, there is a possibility of deformation or phase variation within their structure. [ 43–47 ] To evaluate the structural stability and determine potential phase transitions under varying pressures denoted as “P” ranging from 0 GPa to 80 GPa in Equations (1–5), the material stability criteria, based on elastic constants, is utilized. [ 48 ] false(C44,0.28emC11,0.28emand0.28emnormalBfalse)>0$$\begin{equation}({{C}_{44}},\;{{C}_{11}},\;{\mathrm{and}}\;{\mathrm{B}}) > 0\end{equation}$$ false(C11goodbreak−C12false)>0$$\begin{equation} ({{C}_{11}} - {{C}_{12}}) > 0\end{equation}$$ ()normalC11+2normalC123+P3badbreak>0$$\begin{equation}\left( {\frac{{\left( {{{{\mathrm{C}}}_{11}} + 2{{{\mathrm{C}}}_{12}}} \right)}}{3} + \frac{{\mathrm{P}}}{3}} \right) > 0\end{equation}$$ C44badbreak−normalPgoodbreak>0$$\begin{equation}{{{\mathrm{C}}}_{44}} - {\mathrm{P}} > 0\end{equation}$$ ()normalC11normalC122normalPbadbreak>0$$\begin{equation}\left( {\frac{{\left( {{{{\mathrm{C}}}_{11}} - {{{\mathrm{C}}}_{12}}} \right)}}{2} - {\mathrm{P}}} \right) > 0\end{equation}$$…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…When materials undergo high pressure, there is a possibility of deformation or phase variation within their structure. [ 43–47 ] To evaluate the structural stability and determine potential phase transitions under varying pressures denoted as “P” ranging from 0 GPa to 80 GPa in Equations (1–5), the material stability criteria, based on elastic constants, is utilized. [ 48 ] false(C44,0.28emC11,0.28emand0.28emnormalBfalse)>0$$\begin{equation}({{C}_{44}},\;{{C}_{11}},\;{\mathrm{and}}\;{\mathrm{B}}) > 0\end{equation}$$ false(C11goodbreak−C12false)>0$$\begin{equation} ({{C}_{11}} - {{C}_{12}}) > 0\end{equation}$$ ()normalC11+2normalC123+P3badbreak>0$$\begin{equation}\left( {\frac{{\left( {{{{\mathrm{C}}}_{11}} + 2{{{\mathrm{C}}}_{12}}} \right)}}{3} + \frac{{\mathrm{P}}}{3}} \right) > 0\end{equation}$$ C44badbreak−normalPgoodbreak>0$$\begin{equation}{{{\mathrm{C}}}_{44}} - {\mathrm{P}} > 0\end{equation}$$ ()normalC11normalC122normalPbadbreak>0$$\begin{equation}\left( {\frac{{\left( {{{{\mathrm{C}}}_{11}} - {{{\mathrm{C}}}_{12}}} \right)}}{2} - {\mathrm{P}}} \right) > 0\end{equation}$$…”
Section: Resultsmentioning
confidence: 99%
“…[40][41][42] When materials undergo high pressure, there is a possibility of deformation or phase variation within their structure. [43][44][45][46][47] To evaluate the structural stability and determine potential phase transitions under varying pressures denoted as "P" ranging from 0 GPa to 80 GPa in Equations (1-5), the material stability criteria, based on elastic constants, is utilized. [48] (C 44 , C 11 , and B) > 0…”
Section: Structural and Mechanical Properties Of Bapbomentioning
confidence: 99%
“…Through modulation of strain, materials can exhibit remarkable mechano–electrochemical coupling due to their adaptable properties, by mechanically altering their atomic structures. 27–32 This has the potential to open significant opportunities for achieving exceptional energy-storage capabilities. For instance, according to Yu et al , the presence of local strain at carbon–MoS 2 interfaces with different properties can regulate the energetic pathways in LIBs.…”
Section: Introductionmentioning
confidence: 99%