Onsite matrix elements of the tight-binding Hamiltonian of a strained crystal: Application to silicon, germanium, and their alloys
We discuss a model for the onsite matrix elements of the sp3d5s tight-binding Hamiltonian of a strained diamond or zinc-blende crystal or nanostructure. This model features onsite, off-diagonal couplings among the s, p, and d orbitals and is able to reproduce the effects of arbitrary strains on the...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2009-06, Vol.79 (24), Article 245201 |
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creator | Niquet, Y. M. Rideau, D. Tavernier, C. Jaouen, H. Blase, X. |
description | We discuss a model for the onsite matrix elements of the sp3d5s tight-binding Hamiltonian of a strained diamond or zinc-blende crystal or nanostructure. This model features onsite, off-diagonal couplings among the s, p, and d orbitals and is able to reproduce the effects of arbitrary strains on the band energies and effective masses in the full Brillouin zone. It introduces only a few additional parameters and is free from any ambiguities that might arise from the definition of the macroscopic strains as a function of the atomic positions. We apply this model to silicon, germanium, and their alloys as an illustration. In particular, we make a detailed comparison of tight-binding and ab initio data on strained Si, Ge, and SiGe. |
doi_str_mv | 10.1103/PhysRevB.79.245201 |
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M. ; Rideau, D. ; Tavernier, C. ; Jaouen, H. ; Blase, X.</creator><creatorcontrib>Niquet, Y. M. ; Rideau, D. ; Tavernier, C. ; Jaouen, H. ; Blase, X.</creatorcontrib><description>We discuss a model for the onsite matrix elements of the sp3d5s tight-binding Hamiltonian of a strained diamond or zinc-blende crystal or nanostructure. This model features onsite, off-diagonal couplings among the s, p, and d orbitals and is able to reproduce the effects of arbitrary strains on the band energies and effective masses in the full Brillouin zone. It introduces only a few additional parameters and is free from any ambiguities that might arise from the definition of the macroscopic strains as a function of the atomic positions. We apply this model to silicon, germanium, and their alloys as an illustration. In particular, we make a detailed comparison of tight-binding and ab initio data on strained Si, Ge, and SiGe.</description><identifier>ISSN: 1098-0121</identifier><identifier>EISSN: 1550-235X</identifier><identifier>DOI: 10.1103/PhysRevB.79.245201</identifier><language>eng</language><publisher>American Physical Society</publisher><subject>Computational Physics ; Physics</subject><ispartof>Physical review. 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M.</creatorcontrib><creatorcontrib>Rideau, D.</creatorcontrib><creatorcontrib>Tavernier, C.</creatorcontrib><creatorcontrib>Jaouen, H.</creatorcontrib><creatorcontrib>Blase, X.</creatorcontrib><title>Onsite matrix elements of the tight-binding Hamiltonian of a strained crystal: Application to silicon, germanium, and their alloys</title><title>Physical review. B, Condensed matter and materials physics</title><description>We discuss a model for the onsite matrix elements of the sp3d5s tight-binding Hamiltonian of a strained diamond or zinc-blende crystal or nanostructure. This model features onsite, off-diagonal couplings among the s, p, and d orbitals and is able to reproduce the effects of arbitrary strains on the band energies and effective masses in the full Brillouin zone. It introduces only a few additional parameters and is free from any ambiguities that might arise from the definition of the macroscopic strains as a function of the atomic positions. We apply this model to silicon, germanium, and their alloys as an illustration. In particular, we make a detailed comparison of tight-binding and ab initio data on strained Si, Ge, and SiGe.</description><subject>Computational Physics</subject><subject>Physics</subject><issn>1098-0121</issn><issn>1550-235X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNo9kEFLwzAUx4soOKdfwFOuwjqTl6RNvU1RJwwmouCtvLbpGmnTkcRhr35yV6ae3nt_fu9_-EXRJaNzxii_fm4G_6J3t_M0m4OQQNlRNGFS0hi4fD_e7zRTMWXATqMz7z8oZSITMIm-19aboEmHwZkvolvdaRs86WsSGk2C2TQhLoytjN2QJXamDb01aEcAiQ8OjdUVKd3gA7Y3ZLHdtqbEYHpLQk-82V-9nZGNdh1a89nNCNpq7DaOYNv2gz-PTmpsvb74ndPo7eH-9W4Zr9aPT3eLVVyCYiFmEkopoBC8SBA0ZFAKkaaAiSiglklVguSK16AKVSlVQMElFwWmEqQWivNpdHXobbDNt8506Ia8R5MvF6t8zCjNMkh5smN7Fg5s6Xrvna7_HxjNR-P5n_E8zfKDcf4DYgN26A</recordid><startdate>20090602</startdate><enddate>20090602</enddate><creator>Niquet, Y. 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M.</creatorcontrib><creatorcontrib>Rideau, D.</creatorcontrib><creatorcontrib>Tavernier, C.</creatorcontrib><creatorcontrib>Jaouen, H.</creatorcontrib><creatorcontrib>Blase, X.</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Physical review. B, Condensed matter and materials physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Niquet, Y. M.</au><au>Rideau, D.</au><au>Tavernier, C.</au><au>Jaouen, H.</au><au>Blase, X.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Onsite matrix elements of the tight-binding Hamiltonian of a strained crystal: Application to silicon, germanium, and their alloys</atitle><jtitle>Physical review. B, Condensed matter and materials physics</jtitle><date>2009-06-02</date><risdate>2009</risdate><volume>79</volume><issue>24</issue><artnum>245201</artnum><issn>1098-0121</issn><eissn>1550-235X</eissn><abstract>We discuss a model for the onsite matrix elements of the sp3d5s tight-binding Hamiltonian of a strained diamond or zinc-blende crystal or nanostructure. This model features onsite, off-diagonal couplings among the s, p, and d orbitals and is able to reproduce the effects of arbitrary strains on the band energies and effective masses in the full Brillouin zone. It introduces only a few additional parameters and is free from any ambiguities that might arise from the definition of the macroscopic strains as a function of the atomic positions. We apply this model to silicon, germanium, and their alloys as an illustration. In particular, we make a detailed comparison of tight-binding and ab initio data on strained Si, Ge, and SiGe.</abstract><pub>American Physical Society</pub><doi>10.1103/PhysRevB.79.245201</doi><orcidid>https://orcid.org/0000-0002-0201-9093</orcidid></addata></record> |
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title | Onsite matrix elements of the tight-binding Hamiltonian of a strained crystal: Application to silicon, germanium, and their alloys |
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