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{"title":"Unraveling mechanical and electronic attributes of MN4 (M= Be, Mg, Zn, Cd) monolayers with anisotropic Dirac cone and their excellent supercapacitive performances","authors":"Krishnanshu Basak, Arka Bandyopadhyay, Debnarayan Jana","doi":"10.1016/j.apsusc.2025.163250","DOIUrl":null,"url":null,"abstract":"The recent experimental realization of <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">B</mi><mi is=\"true\">e</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.322ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -763.5 2483.4 999.8\" width=\"5.768ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-42\"></use></g><g is=\"true\" transform=\"translate(759,0)\"><use xlink:href=\"#MJMATHI-65\"></use></g><g is=\"true\" transform=\"translate(1226,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">B</mi><mi is=\"true\">e</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> monolayer, beryllonitrene (Phys. Rev. Lett. 126(2021), 175501), has unveiled a novel group of nitrogen-rich 2D materials, namely <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">M</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.322ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -763.5 2308.9 999.8\" width=\"5.363ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4D\"></use></g><g is=\"true\" transform=\"translate(1051,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">M</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> (M = Be, Mg, Zn, Cd). In this present work, we theoretically explore the anisotropic mechanical and electronic responses of all systems based on the first principles calculations. Among the structures, <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">B</mi><mi is=\"true\">e</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.322ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -763.5 2483.4 999.8\" width=\"5.768ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-42\"></use></g><g is=\"true\" transform=\"translate(759,0)\"><use xlink:href=\"#MJMATHI-65\"></use></g><g is=\"true\" transform=\"translate(1226,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">B</mi><mi is=\"true\">e</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> and <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">M</mi><mi is=\"true\">g</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.458ex\" role=\"img\" style=\"vertical-align: -0.685ex;\" viewbox=\"0 -763.5 2789.4 1058.4\" width=\"6.479ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4D\"></use></g><g is=\"true\" transform=\"translate(1051,0)\"><use xlink:href=\"#MJMATHI-67\"></use></g><g is=\"true\" transform=\"translate(1532,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">M</mi><mi is=\"true\">g</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> sheets are brittle while <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">Z</mi><mi is=\"true\">n</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.322ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -763.5 2581.4 999.8\" width=\"5.996ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-5A\"></use></g><g is=\"true\" transform=\"translate(723,0)\"><use xlink:href=\"#MJMATHI-6E\"></use></g><g is=\"true\" transform=\"translate(1324,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">Z</mi><mi is=\"true\">n</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> and <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.458ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -822.1 2541.4 1058.4\" width=\"5.903ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-43\"></use></g><g is=\"true\" transform=\"translate(760,0)\"><use xlink:href=\"#MJMATHI-64\"></use></g><g is=\"true\" transform=\"translate(1284,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> are ductile in response to external strain along particular direction. Electronic band structure analysis reveals that all the structures exhibit anisotropic Dirac cones like features. We further propose a simple coupled-chain model to investigate the occurrence and robustness of such Dirac cones, thus validating our numerical results. In addition, the capacitive responses of all structures are probed by computing quantum capacitance for different electrochemical potential ranges and identifying <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.458ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -822.1 2541.4 1058.4\" width=\"5.903ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-43\"></use></g><g is=\"true\" transform=\"translate(760,0)\"><use xlink:href=\"#MJMATHI-64\"></use></g><g is=\"true\" transform=\"translate(1284,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> with the maximum value of 219 <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">μ</mi><mi is=\"true\">F</mi><mo is=\"true\">/</mo><mi is=\"true\">c</mi><msup is=\"true\"><mrow is=\"true\"><mi is=\"true\">m</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msup></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"3.002ex\" role=\"img\" style=\"vertical-align: -0.821ex;\" viewbox=\"0 -939.3 3619.4 1292.7\" width=\"8.406ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g><g is=\"true\" transform=\"translate(603,0)\"><use xlink:href=\"#MJMATHI-46\"></use></g><g is=\"true\" transform=\"translate(1353,0)\"><use xlink:href=\"#MJMAIN-2F\"></use></g><g is=\"true\" transform=\"translate(1853,0)\"><use xlink:href=\"#MJMATHI-63\"></use></g><g is=\"true\" transform=\"translate(2287,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-6D\"></use></g></g><g is=\"true\" transform=\"translate(878,362)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-32\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">μ</mi><mi is=\"true\">F</mi><mo is=\"true\">/</mo><mi is=\"true\">c</mi><msup is=\"true\"><mrow is=\"true\"><mi is=\"true\">m</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msup></mrow></math></script></span> for positive electrode potential. The adaptability of a particular electrode as cathode or anode is confirmed by evaluating surface charge density i.e. <span><span style=\"\"><math><mfrac is=\"true\"><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">a</mi></mrow></msub></mrow><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">c</mi></mrow></msub></mrow></mfrac></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"4.363ex\" role=\"img\" style=\"vertical-align: -1.637ex;\" viewbox=\"0 -1173.6 1255.1 1878.5\" width=\"2.915ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g transform=\"translate(120,0)\"><rect height=\"60\" stroke=\"none\" width=\"1015\" x=\"0\" y=\"220\"></rect><g is=\"true\" transform=\"translate(60,588)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-51\"></use></g></g><g is=\"true\" transform=\"translate(559,-163)\"><g is=\"true\"><use transform=\"scale(0.5)\" xlink:href=\"#MJMATHI-61\"></use></g></g></g></g><g is=\"true\" transform=\"translate(84,-419)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-51\"></use></g></g><g is=\"true\" transform=\"translate(559,-163)\"><g is=\"true\"><use transform=\"scale(0.5)\" xlink:href=\"#MJMATHI-63\"></use></g></g></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mfrac is=\"true\"><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">a</mi></mrow></msub></mrow><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">c</mi></mrow></msub></mrow></mfrac></math></script></span>. The numerical results clearly demonstrate that the most prominent value of <span><span style=\"\"><math><mfrac is=\"true\"><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">a</mi></mrow></msub></mrow><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">c</mi></mrow></msub></mrow></mfrac></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"4.363ex\" role=\"img\" style=\"vertical-align: -1.637ex;\" viewbox=\"0 -1173.6 1255.1 1878.5\" width=\"2.915ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g transform=\"translate(120,0)\"><rect height=\"60\" stroke=\"none\" width=\"1015\" x=\"0\" y=\"220\"></rect><g is=\"true\" transform=\"translate(60,588)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-51\"></use></g></g><g is=\"true\" transform=\"translate(559,-163)\"><g is=\"true\"><use transform=\"scale(0.5)\" xlink:href=\"#MJMATHI-61\"></use></g></g></g></g><g is=\"true\" transform=\"translate(84,-419)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-51\"></use></g></g><g is=\"true\" transform=\"translate(559,-163)\"><g is=\"true\"><use transform=\"scale(0.5)\" xlink:href=\"#MJMATHI-63\"></use></g></g></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mfrac is=\"true\"><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">a</mi></mrow></msub></mrow><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">c</mi></mrow></msub></mrow></mfrac></math></script></span> is recorded for <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.458ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -822.1 2541.4 1058.4\" width=\"5.903ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-43\"></use></g><g is=\"true\" transform=\"translate(760,0)\"><use xlink:href=\"#MJMATHI-64\"></use></g><g is=\"true\" transform=\"translate(1284,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> monolayer (2.13), whereas other <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">M</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.322ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -763.5 2308.9 999.8\" width=\"5.363ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4D\"></use></g><g is=\"true\" transform=\"translate(1051,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">M</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> analogues emerge as promising electrodes for symmetric supercapacitors (<span><span style=\"\"><math><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">a</mi></mrow></msub><mo is=\"true\" linebreak=\"goodbreak\" linebreakstyle=\"after\">≈</mo><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">c</mi></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.73ex\" role=\"img\" style=\"vertical-align: -0.821ex;\" viewbox=\"0 -822.1 3798 1175.6\" width=\"8.821ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-51\"></use></g></g><g is=\"true\" transform=\"translate(791,-231)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-61\"></use></g></g></g><g is=\"true\" transform=\"translate(1543,0)\"><use xlink:href=\"#MJMAIN-2248\"></use></g><g is=\"true\" transform=\"translate(2599,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-51\"></use></g></g><g is=\"true\" transform=\"translate(791,-231)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-63\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">a</mi></mrow></msub><mo linebreak=\"goodbreak\" linebreakstyle=\"after\" is=\"true\">≈</mo><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow><mrow is=\"true\"><mi is=\"true\">c</mi></mrow></msub></mrow></math></script></span>). We have also traced out the average value of <span><span style=\"\"><math><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">C</mi></mrow><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow></msub></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.73ex\" role=\"img\" style=\"vertical-align: -0.821ex;\" viewbox=\"0 -822.1 1375.2 1175.6\" width=\"3.194ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-43\"></use></g></g><g is=\"true\" transform=\"translate(715,-155)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-51\"></use></g></g></g></g></svg></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">C</mi></mrow><mrow is=\"true\"><mi is=\"true\">Q</mi></mrow></msub></math></script></span> for both aqueous and ionic/organic systems and <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.458ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -822.1 2541.4 1058.4\" width=\"5.903ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-43\"></use></g><g is=\"true\" transform=\"translate(760,0)\"><use xlink:href=\"#MJMATHI-64\"></use></g><g is=\"true\" transform=\"translate(1284,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">C</mi><mi is=\"true\">d</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> is found to exhibit maximum value of 65 <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">μ</mi><mi is=\"true\">F</mi><mo is=\"true\">/</mo><mi is=\"true\">c</mi><msup is=\"true\"><mrow is=\"true\"><mi is=\"true\">m</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msup></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"3.002ex\" role=\"img\" style=\"vertical-align: -0.821ex;\" viewbox=\"0 -939.3 3619.4 1292.7\" width=\"8.406ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g><g is=\"true\" transform=\"translate(603,0)\"><use xlink:href=\"#MJMATHI-46\"></use></g><g is=\"true\" transform=\"translate(1353,0)\"><use xlink:href=\"#MJMAIN-2F\"></use></g><g is=\"true\" transform=\"translate(1853,0)\"><use xlink:href=\"#MJMATHI-63\"></use></g><g is=\"true\" transform=\"translate(2287,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-6D\"></use></g></g><g is=\"true\" transform=\"translate(878,362)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-32\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">μ</mi><mi is=\"true\">F</mi><mo is=\"true\">/</mo><mi is=\"true\">c</mi><msup is=\"true\"><mrow is=\"true\"><mi is=\"true\">m</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msup></mrow></math></script></span> for higher electrochemical ranges. Moreover, significant improvement in quantum capacitance is reported for metal atom adsorbed <span><span style=\"\"><math><mrow is=\"true\"><mi is=\"true\">B</mi><mi is=\"true\">e</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></span><span style=\"font-size: 90%; display: inline-block;\" tabindex=\"0\"><svg focusable=\"false\" height=\"2.322ex\" role=\"img\" style=\"vertical-align: -0.549ex;\" viewbox=\"0 -763.5 2483.4 999.8\" width=\"5.768ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-42\"></use></g><g is=\"true\" transform=\"translate(759,0)\"><use xlink:href=\"#MJMATHI-65\"></use></g><g is=\"true\" transform=\"translate(1226,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-4E\"></use></g></g><g is=\"true\" transform=\"translate(803,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g></g></g></svg></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">B</mi><mi is=\"true\">e</mi><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">N</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub></mrow></math></script></span> structure at positive electrode potential. These explorations are expected to encourage future research in developing novel and intriguing nanoelectronics and energy storage devices.","PeriodicalId":247,"journal":{"name":"Applied Surface Science","volume":"77 1","pages":""},"PeriodicalIF":6.3000,"publicationDate":"2025-04-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Surface Science","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.apsusc.2025.163250","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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Abstract
The recent experimental realization of
B e N 4 monolayer, beryllonitrene (Phys. Rev. Lett. 126(2021), 175501), has unveiled a novel group of nitrogen-rich 2D materials, namely
M N 4 (M = Be, Mg, Zn, Cd). In this present work, we theoretically explore the anisotropic mechanical and electronic responses of all systems based on the first principles calculations. Among the structures,
B e N 4 and
M g N 4 sheets are brittle while
Z n N 4 and
C d N 4 are ductile in response to external strain along particular direction. Electronic band structure analysis reveals that all the structures exhibit anisotropic Dirac cones like features. We further propose a simple coupled-chain model to investigate the occurrence and robustness of such Dirac cones, thus validating our numerical results. In addition, the capacitive responses of all structures are probed by computing quantum capacitance for different electrochemical potential ranges and identifying
C d N 4 with the maximum value of 219
μ F / c m 2 for positive electrode potential. The adaptability of a particular electrode as cathode or anode is confirmed by evaluating surface charge density i.e.
Q a Q c . The numerical results clearly demonstrate that the most prominent value of
Q a Q c is recorded for
C d N 4 monolayer (2.13), whereas other
M N 4 analogues emerge as promising electrodes for symmetric supercapacitors (
Q a ≈ Q c ). We have also traced out the average value of
C Q for both aqueous and ionic/organic systems and
C d N 4 is found to exhibit maximum value of 65
μ F / c m 2 for higher electrochemical ranges. Moreover, significant improvement in quantum capacitance is reported for metal atom adsorbed
B e N 4 structure at positive electrode potential. These explorations are expected to encourage future research in developing novel and intriguing nanoelectronics and energy storage devices.