4.8 Article

Inverse correlation between quasiparticle mass and Tc in a cuprate high-Tc superconductor

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SCIENCE ADVANCES
卷 2, 期 3, 页码 -

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AMER ASSOC ADVANCEMENT SCIENCE
DOI: 10.1126/sciadv.1501657

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  1. Engineering and Physical Sciences Research Council [EP/K016709/1]
  2. French National Research Agency (ANR) SUPERFIELD
  3. European Magnetic Field Laboratory
  4. LABEX NEXT
  5. High Field Magnet Laboratory, Radboud University Fundamental Research on Matter
  6. EPSRC [EP/L025736/1, EP/K016709/1] Funding Source: UKRI
  7. Engineering and Physical Sciences Research Council [EP/K016709/1, EP/L025736/1, 1363766] Funding Source: researchfish

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Close to a zero-temperature transition between ordered and disordered electronic phases, quantum fluctuations can lead to a strong enhancement of electron mass and to the emergence of competing phases such as superconductivity. A correlation between the existence of such a quantum phase transition and superconductivity is quite well established in some heavy fermion and iron-based superconductors, and there have been suggestions that high-temperature superconductivity in copper-oxide materials (cuprates) may also be driven by the same mechanism. Close to optimal doping, where the superconducting transition temperature T-c is maximal in cuprates, two different phases are known to compete with superconductivity: a poorly understood pseudogap phase and a charge-ordered phase. Recent experiments have shown a strong increase in quasiparticle mass m* in the cuprate YBa2Cu3O7-delta as optimal doping is approached, suggesting that quantum fluctuations of the charge-ordered phase may be responsible for the high-T-c superconductivity. We have tested the robustness of this correlation betweenm* and T-c by performing quantum oscillation studies on the stoichiometric compound YBa2Cu4O8 under hydrostatic pressure. In contrast to the results for YBa2Cu3O7-delta, we find that in YBa(2)Cu4O8, the mass decreases as T-c increases under pressure. This inverse correlation between m* and T-c suggests that quantum fluctuations of the charge order enhance m* but do not enhance T-c.

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