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The origin of the 60 K plateau in YBa2Cu3O6+x
A model for the charge transfer mechanism in YBa2Cu3O6+x high-Tc cuprate based on the critical chain length concept is proposed to account for the 60 and 90 K plateaus in the Tc(x) dependence. It has been shown that, when the statistics of CuO chain formation was described in terms of the two-dimens...
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Published in: | Journal of physics. Condensed matter 2007-08, Vol.19 (34), p.346230-346230 (9) |
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container_end_page | 346230 (9) |
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container_title | Journal of physics. Condensed matter |
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creator | Matic, V M Lazarov, N Dj |
description | A model for the charge transfer mechanism in YBa2Cu3O6+x high-Tc cuprate based on the critical chain length concept is proposed to account for the 60 and 90 K plateaus in the Tc(x) dependence. It has been shown that, when the statistics of CuO chain formation was described in terms of the two-dimensional asymmetric next-to-nearest neighbor Ising (ASYNNNI) model, at any constant temperature below the top of ortho-II phase there exists a uniquely defined value of critical chain length lcr(T) that yields a constant doping p(x)const over the regime of ortho-II phase (related to the 60 K plateau of Tc(x)), while the 90 K plateau coincides with the monotonically increasing p(x) over the optimal doping level p = 0.16 in the regime of the ortho-I phase. Short length chains (l=lcr(T)), are taken as not capable of attracting electrons from CuO2 planes. It is shown that only a part (41%) of the remaining l-lcr(T)+1 holes in the long chains can capture electrons. The results obtained indicate that the ASYNNNI model and two-plateau-like behavior of Tc(x) in YBa2Cu3O6+x are closely connected. |
doi_str_mv | 10.1088/0953-8984/19/34/346230 |
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It has been shown that, when the statistics of CuO chain formation was described in terms of the two-dimensional asymmetric next-to-nearest neighbor Ising (ASYNNNI) model, at any constant temperature below the top of ortho-II phase there exists a uniquely defined value of critical chain length lcr(T) that yields a constant doping p(x)const over the regime of ortho-II phase (related to the 60 K plateau of Tc(x)), while the 90 K plateau coincides with the monotonically increasing p(x) over the optimal doping level p = 0.16 in the regime of the ortho-I phase. Short length chains (l=lcr(T)), are taken as not capable of attracting electrons from CuO2 planes. It is shown that only a part (41%) of the remaining l-lcr(T)+1 holes in the long chains can capture electrons. 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It has been shown that, when the statistics of CuO chain formation was described in terms of the two-dimensional asymmetric next-to-nearest neighbor Ising (ASYNNNI) model, at any constant temperature below the top of ortho-II phase there exists a uniquely defined value of critical chain length lcr(T) that yields a constant doping p(x)const over the regime of ortho-II phase (related to the 60 K plateau of Tc(x)), while the 90 K plateau coincides with the monotonically increasing p(x) over the optimal doping level p = 0.16 in the regime of the ortho-I phase. Short length chains (l=lcr(T)), are taken as not capable of attracting electrons from CuO2 planes. It is shown that only a part (41%) of the remaining l-lcr(T)+1 holes in the long chains can capture electrons. The results obtained indicate that the ASYNNNI model and two-plateau-like behavior of Tc(x) in YBa2Cu3O6+x are closely connected.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Cuprates superconductors (high tc and insulating parent compounds)</subject><subject>Effects of material synthesis, crystal structure, and chemical composition</subject><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Superconductivity</subject><subject>Transition temperature variations</subject><subject>Y-based cuprates</subject><issn>0953-8984</issn><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><recordid>eNptkEtLAzEQgIMoWKt_QfaiF4mdJJM0OWrxhYVeKugpZLdZjWy762YX9N-bpUUPCgPz-mYOHyGnDC4ZaD0BIwXVRuOEmYnAFIoL2CMjJhSjCvXzPhn9QIfkKMZ3AEAtcETo8s1ndRtewyary6xLnYLsMWsq13nXZ2n8cu34rBcLdfF5TA5KV0V_sstj8nR7s5zd0_ni7mF2NaeBc9VRWTKHDM0K88LkAnWqUTglS4VeSpErbzyb5iCL3GsEjjmXK-SKq0IbxsSYnG__Nm390fvY2XWIha8qt_F1H60AxiQqSODZDnSxcFXZuk0Rom3asHbtl2UGOJ_iwLEtF-rmdwt2EGgHN3Zwk3gr0G4Fphv69-Z_1jarUnwDQX5sJA</recordid><startdate>20070829</startdate><enddate>20070829</enddate><creator>Matic, V M</creator><creator>Lazarov, N Dj</creator><general>IOP Publishing</general><general>Institute of Physics</general><scope>IQODW</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20070829</creationdate><title>The origin of the 60 K plateau in YBa2Cu3O6+x</title><author>Matic, V M ; Lazarov, N Dj</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i226t-5f1a4149d4bc9b34814943a65f64e553b6e9e17b05cbe84024b25d42626c89113</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Cuprates superconductors (high tc and insulating parent compounds)</topic><topic>Effects of material synthesis, crystal structure, and chemical composition</topic><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Superconductivity</topic><topic>Transition temperature variations</topic><topic>Y-based cuprates</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Matic, V M</creatorcontrib><creatorcontrib>Lazarov, N Dj</creatorcontrib><collection>Pascal-Francis</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Matic, V M</au><au>Lazarov, N Dj</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The origin of the 60 K plateau in YBa2Cu3O6+x</atitle><jtitle>Journal of physics. Condensed matter</jtitle><date>2007-08-29</date><risdate>2007</risdate><volume>19</volume><issue>34</issue><spage>346230</spage><epage>346230 (9)</epage><pages>346230-346230 (9)</pages><issn>0953-8984</issn><eissn>1361-648X</eissn><coden>JCOMEL</coden><abstract>A model for the charge transfer mechanism in YBa2Cu3O6+x high-Tc cuprate based on the critical chain length concept is proposed to account for the 60 and 90 K plateaus in the Tc(x) dependence. It has been shown that, when the statistics of CuO chain formation was described in terms of the two-dimensional asymmetric next-to-nearest neighbor Ising (ASYNNNI) model, at any constant temperature below the top of ortho-II phase there exists a uniquely defined value of critical chain length lcr(T) that yields a constant doping p(x)const over the regime of ortho-II phase (related to the 60 K plateau of Tc(x)), while the 90 K plateau coincides with the monotonically increasing p(x) over the optimal doping level p = 0.16 in the regime of the ortho-I phase. Short length chains (l=lcr(T)), are taken as not capable of attracting electrons from CuO2 planes. It is shown that only a part (41%) of the remaining l-lcr(T)+1 holes in the long chains can capture electrons. The results obtained indicate that the ASYNNNI model and two-plateau-like behavior of Tc(x) in YBa2Cu3O6+x are closely connected.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/0953-8984/19/34/346230</doi></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Cuprates superconductors (high tc and insulating parent compounds) Effects of material synthesis, crystal structure, and chemical composition Exact sciences and technology Physics Superconductivity Transition temperature variations Y-based cuprates |
title | The origin of the 60 K plateau in YBa2Cu3O6+x |
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