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        <datestamp>2026-09-15T20:42:46Z</datestamp>
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          <dc:title>Data for Linear-in temperature resistivity from an isotropic Planckian scattering rate</dc:title>
          <dc:creator>Gaël Grissonnanche (24956347)</dc:creator>
          <dc:creator>Yawen Fang (17493939)</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>Jianshi Zhou (1753051)</dc:creator>
          <dc:creator>David Graf (1776046)</dc:creator>
          <dc:creator>Paul Goddard (564595)</dc:creator>
          <dc:creator>Louis Taillefer (24956362)</dc:creator>
          <dc:creator>B. J. Ramshaw (10738750)</dc:creator>
          <dc:subject>Condensed matter</dc:subject>
          <dc:subject>Superconductivity</dc:subject>
          <dc:subject>Particles (Nuclear physics)</dc:subject>
          <dc:subject>Migrated from ePrints</dc:subject>
          <dc:description>A variety of ‘strange metals’ exhibit resistivity that decreases linearly with temperature as the temperature decreases to zero1,2,3, in contrast to conventional metals where resistivity decreases quadratically with temperature. This linear-in-temperature resistivity has been attributed to charge carriers scattering at a rate given by ħ/τ = αkBT, where α is a constant of order unity, ħ is the Planck constant and kB is the Boltzmann constant. This simple relationship between the scattering rate and temperature is observed across a wide variety of materials, suggesting a fundamental upper limit on scattering—the ‘Planckian limit’4,5—but little is known about the underlying origins of this limit. Here we report a measurement of the angle-dependent magnetoresistance of La1.6−xNd0.4SrxCuO4—a hole-doped cuprate that shows linear-in-temperature resistivity down to the lowest measured temperatures6. The angle-dependent magnetoresistance shows a well defined Fermi surface that agrees quantitatively with angle-resolved photoemission spectroscopy measurements7 and reveals a linear-in-temperature scattering rate that saturates at the Planckian limit, namely α = 1.2 ± 0.4. Remarkably, we find that this Planckian scattering rate is isotropic, that is, it is independent of direction, in contrast to expectations from ‘hotspot’ models8,9. Our findings suggest that linear-in-temperature resistivity in strange metals emerges from a momentum-independent inelastic scattering rate that reaches the Planckian limit.&lt;br&gt;&lt;br&gt;The archive contains the experimental data from the following figures:  Figure 2a Extended Data (ED) Figure 1b Extended Data (ED) Figure 5a  The rho_xx and rho_zz data shown in Figure 3 are published in  DOI: 10.1016/j.physc.2009.11.073 DOI: 10.1038/NPHYS1109   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>2021-07-29T00:00:00Z</dc:date>
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          <dc:identifier>10.82444/warw.33822934.v1</dc:identifier>
          <dc:relation>https://figshare.com/articles/dataset/Data_for_Linear-in_temperature_resistivity_from_an_isotropic_Planckian_scattering_rate/33822934</dc:relation>
          <dc:rights>CC BY 4.0</dc:rights>
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