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        <datestamp>2026-09-16T09:09:25Z</datestamp>
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          <dc:title>Data for Fermi surface transformation at the pseudogap critical point of a cuprate superconductor</dc:title>
          <dc:creator>Yawen Fang (17493939)</dc:creator>
          <dc:creator>Gaël Grissonnanche (24956347)</dc:creator>
          <dc:creator>Anaëlle Legros (24956350)</dc:creator>
          <dc:creator>Simon Verret (24956353)</dc:creator>
          <dc:creator>Francis Laliberte (24956356)</dc:creator>
          <dc:creator>Clément Collignon (24956359)</dc:creator>
          <dc:creator>Amirreza Ataei (24969058)</dc:creator>
          <dc:creator>Maxime Dion (24969061)</dc:creator>
          <dc:creator>Jianshi Zhou (1753051)</dc:creator>
          <dc:creator>David Graf (1776046)</dc:creator>
          <dc:creator>M. J. Lawler (24969064)</dc:creator>
          <dc:creator>Paul A. Goddard (1422469)</dc:creator>
          <dc:creator>Louis Taillefer (24956362)</dc:creator>
          <dc:creator>B. J. Ramshaw (10738750)</dc:creator>
          <dc:subject>Fermi surfaces</dc:subject>
          <dc:subject>High temperature superconductivity</dc:subject>
          <dc:subject>Magnetoresistance</dc:subject>
          <dc:subject>Semiconductor doping</dc:subject>
          <dc:subject>Energy gap (Physics)</dc:subject>
          <dc:subject>Migrated from ePrints</dc:subject>
          <dc:description>The nature of the pseudogap phase remains a major puzzle in our understanding of cuprate high-temperature superconductivity. Whether or not this metallic phase is defined by any of the reported broken symmetries, the topology of its Fermi surface remains a fundamental open question. Here we use angle-dependent magnetoresistance (ADMR) to measure the Fermi surface of the La1.6–xNd0.4SrxCuO4 cuprate. Outside the pseudogap phase, we fit the ADMR data and extract a Fermi surface geometry that is in excellent agreement with angle-resolved photoemission data. Within the pseudogap phase, the ADMR is qualitatively different, revealing a transformation of the Fermi surface. We can rule out changes in the quasiparticle lifetime as the sole cause of this transformation. We find that our data are most consistent with a pseudogap Fermi surface that consists of small, nodal hole pockets, thereby accounting for the drop in carrier density across the pseudogap transition found in several cuprates.&lt;br&gt;&lt;br&gt;The archive contains the experimental data from the following figures:  Figure 1c Figure 1d Figure S3   Data are listed in the archive as follows   Fig??_HxxTyyphizz.dat   where  ?? = the figure number,  xx = the applied magnetic field value in Tesla,  yy = the sample temperature in kelvin, and  zz = the azimuthal angle in degrees.</dc:description>
          <dc:date>2022-03-15T00:00:00Z</dc:date>
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          <dc:identifier>10.82444/warw.33836011.v1</dc:identifier>
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          <dc:rights>CC BY 4.0</dc:rights>
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