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To study whether this geometric concept, i.e., using 2D layers as building blocks for 3D structures, can be applied to computational materials design, we theoretically investigate the dynamical stability of copper-based compounds Cu<jats:italic>X<\/jats:italic> (a metallic element <jats:italic>X<\/jats:italic>) in the B<jats:inline-formula><jats:alternatives><jats:tex-math>$$_h$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mi>h<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> and L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_1$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>1<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> structures constructed from the buckled honeycomb (BHC) structure and in the B2 and L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_0$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>0<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> structures constructed from the buckled square (BSQ) structure. We demonstrate that (i) if Cu<jats:italic>X<\/jats:italic> in the BHC structure is dynamically stable, those in the B<jats:inline-formula><jats:alternatives><jats:tex-math>$$_h$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mi>h<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> and L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_1$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>1<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> structures are also stable. Using molecular dynamics simulations, we particularly show that CuAu in the B<jats:inline-formula><jats:alternatives><jats:tex-math>$$_h$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mi>h<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> and L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_1$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>1<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> structures withstand temperatures as high as 1000\u00a0K. Although the interrelationship of the metastability between the BSQ and the 3D structures (B2 and L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_0$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>0<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>) is not clear, we find that (ii) if Cu<jats:italic>X<\/jats:italic> in the B2 (L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_0$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>0<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>) structure is dynamically stable, that in the L1<jats:inline-formula><jats:alternatives><jats:tex-math>$$_0$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mn>0<\/mml:mn>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> (B2) is unstable. This is rationalized by the tetragonal Bain path calculations.<\/jats:p>","DOI":"10.1038\/s41598-021-94034-6","type":"journal-article","created":{"date-parts":[[2021,7,16]],"date-time":"2021-07-16T10:03:33Z","timestamp":1626429813000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":9,"title":["Metastability relationship between two- and three-dimensional crystal structures: a case study of the Cu-based compounds"],"prefix":"10.1038","volume":"11","author":[{"given":"Shota","family":"Ono","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"297","published-online":{"date-parts":[[2021,7,16]]},"reference":[{"key":"94034_CR1","doi-asserted-by":"publisher","first-page":"106101","DOI":"10.1103\/PhysRevLett.118.106101","volume":"118","author":"M Ashton","year":"2017","unstructured":"Ashton, M., Paul, J., Sinnott, S. B. & Hennig, R. G. 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