Critical Doping for the Onset of Fermi-Surface Reconstruction by Charge-Density-Wave Order in the Cuprate Superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\)
The Seebeck coefficient \(S\) of the cuprate superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\) (LSCO) was measured in magnetic fields large enough to access the normal state at low temperatures, for a range of Sr concentrations from \(x = 0.07\) to \(x = 0.15\). For \(x = 0.11\), 0.12, 0.125 and...
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creator | Badoux, S Afshar, S A A Michon, B Ouellet, A tier, S LeBoeuf, D Croft, T P Lester, C Hayden, S M Takagi, H Yamada, K Graf, D Doiron-Leyraud, N Taillefer, Louis |
description | The Seebeck coefficient \(S\) of the cuprate superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\) (LSCO) was measured in magnetic fields large enough to access the normal state at low temperatures, for a range of Sr concentrations from \(x = 0.07\) to \(x = 0.15\). For \(x = 0.11\), 0.12, 0.125 and 0.13, \(S/T\) decreases upon cooling to become negative at low temperatures. The same behavior is observed in the Hall coefficient \(R_{H}(T)\). In analogy with other hole-doped cuprates at similar hole concentrations \(p\), the negative \(S\) and \(R_{H}\) show that the Fermi surface of LSCO undergoes a reconstruction caused by the onset of charge-density-wave modulations. Such modulations have indeed been detected in LSCO by X-ray diffraction in precisely the same doping range. Our data show that in LSCO this Fermi-surface reconstruction is confined to \(0.085 < p < 0.15\). We argue that in the field-induced normal state of LSCO, charge-density-wave order ends at a critical doping \(p_{\rm CDW} = 0.15 \pm 0.005\), well below the pseudogap critical doping \(p^\star \simeq 0.19\). |
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For \(x = 0.11\), 0.12, 0.125 and 0.13, \(S/T\) decreases upon cooling to become negative at low temperatures. The same behavior is observed in the Hall coefficient \(R_{H}(T)\). In analogy with other hole-doped cuprates at similar hole concentrations \(p\), the negative \(S\) and \(R_{H}\) show that the Fermi surface of LSCO undergoes a reconstruction caused by the onset of charge-density-wave modulations. Such modulations have indeed been detected in LSCO by X-ray diffraction in precisely the same doping range. Our data show that in LSCO this Fermi-surface reconstruction is confined to \(0.085 < p < 0.15\). We argue that in the field-induced normal state of LSCO, charge-density-wave order ends at a critical doping \(p_{\rm CDW} = 0.15 \pm 0.005\), well below the pseudogap critical doping \(p^\star \simeq 0.19\).</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1512.00292</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Charge density waves ; Cuprates ; Doping ; Fermi surfaces ; Hall effect ; Physics - Strongly Correlated Electrons ; Physics - Superconductivity ; Reconstruction ; Seebeck effect ; X-ray diffraction</subject><ispartof>arXiv.org, 2016-04</ispartof><rights>2016. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,784,885,27923</link.rule.ids><backlink>$$Uhttps://doi.org/10.1103/PhysRevX.6.021004$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.1512.00292$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Badoux, S</creatorcontrib><creatorcontrib>Afshar, S A A</creatorcontrib><creatorcontrib>Michon, B</creatorcontrib><creatorcontrib>Ouellet, A</creatorcontrib><creatorcontrib>tier, S</creatorcontrib><creatorcontrib>LeBoeuf, D</creatorcontrib><creatorcontrib>Croft, T P</creatorcontrib><creatorcontrib>Lester, C</creatorcontrib><creatorcontrib>Hayden, S M</creatorcontrib><creatorcontrib>Takagi, H</creatorcontrib><creatorcontrib>Yamada, K</creatorcontrib><creatorcontrib>Graf, D</creatorcontrib><creatorcontrib>Doiron-Leyraud, N</creatorcontrib><creatorcontrib>Taillefer, Louis</creatorcontrib><title>Critical Doping for the Onset of Fermi-Surface Reconstruction by Charge-Density-Wave Order in the Cuprate Superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\)</title><title>arXiv.org</title><description>The Seebeck coefficient \(S\) of the cuprate superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\) (LSCO) was measured in magnetic fields large enough to access the normal state at low temperatures, for a range of Sr concentrations from \(x = 0.07\) to \(x = 0.15\). For \(x = 0.11\), 0.12, 0.125 and 0.13, \(S/T\) decreases upon cooling to become negative at low temperatures. The same behavior is observed in the Hall coefficient \(R_{H}(T)\). In analogy with other hole-doped cuprates at similar hole concentrations \(p\), the negative \(S\) and \(R_{H}\) show that the Fermi surface of LSCO undergoes a reconstruction caused by the onset of charge-density-wave modulations. Such modulations have indeed been detected in LSCO by X-ray diffraction in precisely the same doping range. Our data show that in LSCO this Fermi-surface reconstruction is confined to \(0.085 < p < 0.15\). We argue that in the field-induced normal state of LSCO, charge-density-wave order ends at a critical doping \(p_{\rm CDW} = 0.15 \pm 0.005\), well below the pseudogap critical doping \(p^\star \simeq 0.19\).</description><subject>Charge density waves</subject><subject>Cuprates</subject><subject>Doping</subject><subject>Fermi surfaces</subject><subject>Hall effect</subject><subject>Physics - Strongly Correlated Electrons</subject><subject>Physics - Superconductivity</subject><subject>Reconstruction</subject><subject>Seebeck effect</subject><subject>X-ray diffraction</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotkMFqwkAQhkOhULE-QE9d6EUPsbuzu0k8lljbgiBUoZdA2GQnuqJJuklEEV-lz9o09jTDzP__M3yO88DoWARS0mdlj-YwZpLBmFKYwI3TA86ZGwiAO2dQVVvazj0fpOQ95ye0pjap2pFpUZp8TbLCknqDZJFXWJMiIzO0e-MuG5upFMknpkVe1bZJa1PkJDmRcKPsGt0p5pWpT-6XOrRmq9ESk3dJYVNaVSNZNiXa1q1bb3tkrqIhic_gHi8kGi1tNIzPXRs2i24jLtHo3rnN1K7CwX_tO6vZ6yp8d-eLt4_wZe4qCeAqigwSqjgKjuArRrUHvtYp1xlXElFIT7KJAsEDKj0mkiSV2k-l4r7OMOB95_Ea28GLS2v2yp7iP4hxB7FVPF0VpS2-G6zqeFs0Nm9_ioH6AQQTIYD_Akf5dS0</recordid><startdate>20160408</startdate><enddate>20160408</enddate><creator>Badoux, S</creator><creator>Afshar, S A A</creator><creator>Michon, B</creator><creator>Ouellet, A</creator><creator>tier, S</creator><creator>LeBoeuf, D</creator><creator>Croft, T P</creator><creator>Lester, C</creator><creator>Hayden, S M</creator><creator>Takagi, H</creator><creator>Yamada, K</creator><creator>Graf, D</creator><creator>Doiron-Leyraud, N</creator><creator>Taillefer, Louis</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20160408</creationdate><title>Critical Doping for the Onset of Fermi-Surface Reconstruction by Charge-Density-Wave Order in the Cuprate Superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\)</title><author>Badoux, S ; Afshar, S A A ; Michon, B ; Ouellet, A ; tier, S ; LeBoeuf, D ; Croft, T P ; Lester, C ; Hayden, S M ; Takagi, H ; Yamada, K ; Graf, D ; Doiron-Leyraud, N ; Taillefer, Louis</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a522-a0e12b0a3e43e27a10d627ddc3df3a5ee456519a243805614bbc5d7c5a37dfe83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Charge density waves</topic><topic>Cuprates</topic><topic>Doping</topic><topic>Fermi surfaces</topic><topic>Hall effect</topic><topic>Physics - Strongly Correlated Electrons</topic><topic>Physics - Superconductivity</topic><topic>Reconstruction</topic><topic>Seebeck effect</topic><topic>X-ray diffraction</topic><toplevel>online_resources</toplevel><creatorcontrib>Badoux, S</creatorcontrib><creatorcontrib>Afshar, S A A</creatorcontrib><creatorcontrib>Michon, B</creatorcontrib><creatorcontrib>Ouellet, A</creatorcontrib><creatorcontrib>tier, S</creatorcontrib><creatorcontrib>LeBoeuf, D</creatorcontrib><creatorcontrib>Croft, T P</creatorcontrib><creatorcontrib>Lester, C</creatorcontrib><creatorcontrib>Hayden, S M</creatorcontrib><creatorcontrib>Takagi, H</creatorcontrib><creatorcontrib>Yamada, K</creatorcontrib><creatorcontrib>Graf, D</creatorcontrib><creatorcontrib>Doiron-Leyraud, N</creatorcontrib><creatorcontrib>Taillefer, Louis</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Badoux, S</au><au>Afshar, S A A</au><au>Michon, B</au><au>Ouellet, A</au><au>tier, S</au><au>LeBoeuf, D</au><au>Croft, T P</au><au>Lester, C</au><au>Hayden, S M</au><au>Takagi, H</au><au>Yamada, K</au><au>Graf, D</au><au>Doiron-Leyraud, N</au><au>Taillefer, Louis</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Critical Doping for the Onset of Fermi-Surface Reconstruction by Charge-Density-Wave Order in the Cuprate Superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\)</atitle><jtitle>arXiv.org</jtitle><date>2016-04-08</date><risdate>2016</risdate><eissn>2331-8422</eissn><abstract>The Seebeck coefficient \(S\) of the cuprate superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\) (LSCO) was measured in magnetic fields large enough to access the normal state at low temperatures, for a range of Sr concentrations from \(x = 0.07\) to \(x = 0.15\). For \(x = 0.11\), 0.12, 0.125 and 0.13, \(S/T\) decreases upon cooling to become negative at low temperatures. The same behavior is observed in the Hall coefficient \(R_{H}(T)\). In analogy with other hole-doped cuprates at similar hole concentrations \(p\), the negative \(S\) and \(R_{H}\) show that the Fermi surface of LSCO undergoes a reconstruction caused by the onset of charge-density-wave modulations. Such modulations have indeed been detected in LSCO by X-ray diffraction in precisely the same doping range. Our data show that in LSCO this Fermi-surface reconstruction is confined to \(0.085 < p < 0.15\). We argue that in the field-induced normal state of LSCO, charge-density-wave order ends at a critical doping \(p_{\rm CDW} = 0.15 \pm 0.005\), well below the pseudogap critical doping \(p^\star \simeq 0.19\).</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1512.00292</doi><oa>free_for_read</oa></addata></record> |
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subjects | Charge density waves Cuprates Doping Fermi surfaces Hall effect Physics - Strongly Correlated Electrons Physics - Superconductivity Reconstruction Seebeck effect X-ray diffraction |
title | Critical Doping for the Onset of Fermi-Surface Reconstruction by Charge-Density-Wave Order in the Cuprate Superconductor La\( _{2-x} \)Sr\(_{x} \)CuO\( _{4}\) |
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