Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition.
Autor(a) principal: | |
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Data de Publicação: | 2012 |
Outros Autores: | |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UFOP |
Texto Completo: | http://www.repositorio.ufop.br/handle/123456789/1646 |
Resumo: | The resistivity as a function of temperature for high temperature superconductors is very unusual and, despite its importance, lacks a unified theoretical explanation. It is linear with the temperature for overdoped compounds but it falls more quickly as the doping level decreases. The resistivity of underdoped cuprates increases like that of an insulator below a characteristic temperature where it shows a minimum. We show that this overall behavior can be explained by calculations using an electronicphase segregation into two main component phases with low and high electronic densities. The total resistance is calculated from the various contributions through several processes of random picking of the local resistivities and using a common statistical random resistor network approach. |
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Pinheiro, Carlos Felipe SaraivaMello, Evandro Vidor Lins de2012-10-16T12:11:35Z2012-10-16T12:11:35Z2012PINHEIRO, C. F. S.; MELLO, E. V. L. de. Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. Physica A: Statistical Mechanics and its Applications, v. 391, n. 4, p. 1532-1539, fev. 2012. Disponível em: <https://www.sciencedirect.com/science/article/pii/S0378437111006613>. Acesso em: 16 out. 2012.03784371http://www.repositorio.ufop.br/handle/123456789/1646The resistivity as a function of temperature for high temperature superconductors is very unusual and, despite its importance, lacks a unified theoretical explanation. It is linear with the temperature for overdoped compounds but it falls more quickly as the doping level decreases. The resistivity of underdoped cuprates increases like that of an insulator below a characteristic temperature where it shows a minimum. We show that this overall behavior can be explained by calculations using an electronicphase segregation into two main component phases with low and high electronic densities. The total resistance is calculated from the various contributions through several processes of random picking of the local resistivities and using a common statistical random resistor network approach.Phase separation transitionHigh critical temperature transitionSuperconductor transitionRandom resistivity networkRandom resistivity network calculations for cuprate superconductors with an electronic phase separation transition.info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleO periódico Physica A concede permissão para depósito do artigo no Repositório Institucional da UFOP. Número da licença: 3345930656208.info:eu-repo/semantics/openAccessengreponame:Repositório Institucional da UFOPinstname:Universidade Federal de Ouro Preto (UFOP)instacron:UFOPLICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://www.repositorio.ufop.br/bitstream/123456789/1646/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD55ORIGINALARTIGO_RandomResistivityNetwork.pdfARTIGO_RandomResistivityNetwork.pdfapplication/pdf570504http://www.repositorio.ufop.br/bitstream/123456789/1646/1/ARTIGO_RandomResistivityNetwork.pdf185e957f32cfcac4cccd0c128d25d8ffMD51123456789/16462019-03-12 13:54:14.117oai:localhost: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Repositório InstitucionalPUBhttp://www.repositorio.ufop.br/oai/requestrepositorio@ufop.edu.bropendoar:32332019-03-12T17:54:14Repositório Institucional da UFOP - Universidade Federal de Ouro Preto (UFOP)false |
dc.title.pt_BR.fl_str_mv |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
title |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
spellingShingle |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. Pinheiro, Carlos Felipe Saraiva Phase separation transition High critical temperature transition Superconductor transition Random resistivity network |
title_short |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
title_full |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
title_fullStr |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
title_full_unstemmed |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
title_sort |
Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. |
author |
Pinheiro, Carlos Felipe Saraiva |
author_facet |
Pinheiro, Carlos Felipe Saraiva Mello, Evandro Vidor Lins de |
author_role |
author |
author2 |
Mello, Evandro Vidor Lins de |
author2_role |
author |
dc.contributor.author.fl_str_mv |
Pinheiro, Carlos Felipe Saraiva Mello, Evandro Vidor Lins de |
dc.subject.por.fl_str_mv |
Phase separation transition High critical temperature transition Superconductor transition Random resistivity network |
topic |
Phase separation transition High critical temperature transition Superconductor transition Random resistivity network |
description |
The resistivity as a function of temperature for high temperature superconductors is very unusual and, despite its importance, lacks a unified theoretical explanation. It is linear with the temperature for overdoped compounds but it falls more quickly as the doping level decreases. The resistivity of underdoped cuprates increases like that of an insulator below a characteristic temperature where it shows a minimum. We show that this overall behavior can be explained by calculations using an electronicphase segregation into two main component phases with low and high electronic densities. The total resistance is calculated from the various contributions through several processes of random picking of the local resistivities and using a common statistical random resistor network approach. |
publishDate |
2012 |
dc.date.accessioned.fl_str_mv |
2012-10-16T12:11:35Z |
dc.date.available.fl_str_mv |
2012-10-16T12:11:35Z |
dc.date.issued.fl_str_mv |
2012 |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
format |
article |
status_str |
publishedVersion |
dc.identifier.citation.fl_str_mv |
PINHEIRO, C. F. S.; MELLO, E. V. L. de. Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. Physica A: Statistical Mechanics and its Applications, v. 391, n. 4, p. 1532-1539, fev. 2012. Disponível em: <https://www.sciencedirect.com/science/article/pii/S0378437111006613>. Acesso em: 16 out. 2012. |
dc.identifier.uri.fl_str_mv |
http://www.repositorio.ufop.br/handle/123456789/1646 |
dc.identifier.issn.none.fl_str_mv |
03784371 |
identifier_str_mv |
PINHEIRO, C. F. S.; MELLO, E. V. L. de. Random resistivity network calculations for cuprate superconductors with an electronic phase separation transition. Physica A: Statistical Mechanics and its Applications, v. 391, n. 4, p. 1532-1539, fev. 2012. Disponível em: <https://www.sciencedirect.com/science/article/pii/S0378437111006613>. Acesso em: 16 out. 2012. 03784371 |
url |
http://www.repositorio.ufop.br/handle/123456789/1646 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
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openAccess |
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UFOP |
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Repositório Institucional da UFOP |
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Repositório Institucional da UFOP |
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