Reconciling scaling of the optical conductivity of cuprate superconductors with Planckian resistivity and specific heat
Materials tuned to a quantum critical point display universal scaling properties as a function of temperature T and frequency ω . A long-standing puzzle regarding cuprate superconductors has been the observed power-law dependence of optical conductivity with an exponent smaller than one, in contrast...
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Veröffentlicht in: | Nature communications 2023-05, Vol.14 (1), p.3033-3033, Article 3033 |
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Sprache: | eng |
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Zusammenfassung: | Materials tuned to a quantum critical point display universal scaling properties as a function of temperature
T
and frequency
ω
. A long-standing puzzle regarding cuprate superconductors has been the observed power-law dependence of optical conductivity with an exponent smaller than one, in contrast to
T
-linear dependence of the resistivity and
ω
-linear dependence of the optical scattering rate. Here, we present and analyze resistivity and optical conductivity of La
2−
x
Sr
x
CuO
4
with
x
= 0.24. We demonstrate
ℏ
ω
/
k
B
T
scaling of the optical data over a wide range of frequency and temperature,
T
-linear resistivity, and optical effective mass proportional to
~
ln
T
corroborating previous specific heat experiments. We show that a
T
,
ω
-linear scaling
Ansatz
for the inelastic scattering rate leads to a unified theoretical description of the experimental data, including the power-law of the optical conductivity. This theoretical framework provides new opportunities for describing the unique properties of quantum critical matter.
A long-standing puzzle in the quantum critical behavior of cuprate superconductors has been the observed sub-linear power-law dependence of optical conductivity. Here, the authors present measurements of the optical spectra and resistivity of La
2−x
Sr
x
CuO
4
, and develop a theoretical framework that yields a unified description of the optical spectra, resistivity and specific heat. |
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ISSN: | 2041-1723 2041-1723 |
DOI: | 10.1038/s41467-023-38762-5 |