<p>The Hall effect of several single crystal and thin-film samples of YBa<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7012_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>Cu<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7012_Article_IEq2.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7012_Article_IEq3.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{6+x}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn>6</mn> <mo>+</mo> <mi>x</mi> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> with different carrier concentration was measured in the temperature interval from <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7012_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(T_{c}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>c</mi> </msub> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7012_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(T = 300 K\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>=</mo> <mn>300</mn> <mi>K</mi> </mrow> </math></EquationSource> </InlineEquation>. In this region, the Hall coefficient decreases exponentially with temperature according to a cut-off law where the characteristic parameter closely reproduces the pseudogap line when plotted as a function of the carrier concentration <i>p</i>. The strongly temperature-dependent Hall coefficient is interpreted in terms of the superposition of ordinary and anomalous Hall terms. The anomalous contribution is related to a Griffiths-type antiferromagnetic configuration that forms at the pseudogap line. The coefficients of the ordinary and anomalous terms show a complex dependence on the carrier concentration, suggesting the occurrence of a Fermi surface reconstruction at <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7012_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\approx 0.14\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>≈</mo> <mn>0.14</mn> </mrow> </math></EquationSource> </InlineEquation>, where electron-type pockets are supposed to stabilize.</p>

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Hall Effect and the Pseudogap in YBa\(_{2}\)Cu\(_{3}\)O\(_{6+x}\)

  • P. A. Sobocinski,
  • O. J. de Freitas,
  • F. Mesquita,
  • P. Grande,
  • J. Schaf,
  • P. Pureur,
  • T. Puig,
  • X. Obradors

摘要

The Hall effect of several single crystal and thin-film samples of YBa \(_{2}\) 2 Cu \(_{3}\) 3 O \(_{6+x}\) 6 + x with different carrier concentration was measured in the temperature interval from \(T_{c}\) T c to \(T = 300 K\) T = 300 K . In this region, the Hall coefficient decreases exponentially with temperature according to a cut-off law where the characteristic parameter closely reproduces the pseudogap line when plotted as a function of the carrier concentration p. The strongly temperature-dependent Hall coefficient is interpreted in terms of the superposition of ordinary and anomalous Hall terms. The anomalous contribution is related to a Griffiths-type antiferromagnetic configuration that forms at the pseudogap line. The coefficients of the ordinary and anomalous terms show a complex dependence on the carrier concentration, suggesting the occurrence of a Fermi surface reconstruction at \(p\approx 0.14\) p 0.14 , where electron-type pockets are supposed to stabilize.