Charge density waves as the origin of dip-hump structures in the differential tunneling conductance of cuprates: The case of d-wave superconductivity

Quasiparticle differential current-voltage characteristics (CVCs) G(V)G(V) of non-symmetric tunnel junctions between d -wave superconductors with charge-density waves (CDWs) and normal metals were calculated. The dependences G(V)G(V) were shown to have a V-like form at small voltages V and low tempe...

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Veröffentlicht in:Physica. C, Superconductivity Superconductivity, 2014-08, Vol.503, p.7-13
Hauptverfasser: GABOVICH, Alexander M, VOITENKO, Alexander I
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description Quasiparticle differential current-voltage characteristics (CVCs) G(V)G(V) of non-symmetric tunnel junctions between d -wave superconductors with charge-density waves (CDWs) and normal metals were calculated. The dependences G(V)G(V) were shown to have a V-like form at small voltages V and low temperatures, and to be asymmetric at larger V owing to the presence of CDW peak in either of the V-branches. The spatial scatter of the dielectric (CDW) order parameter smears the CDW peak into a hump and induces a peak-dip-hump structure (PDHS) typical of CVCs observed for such junctions. At temperatures larger than the superconducting critical one, the PDHS evolves into a pseudogap depression. The results agree well with the scanning tunneling microscopy data for Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) and YBa sub(2)Cu sub(3)O sub(7- delta ). The results differ substantially from those obtained earlier for CDW s-wave superconductors.
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C, Superconductivity</title><description>Quasiparticle differential current-voltage characteristics (CVCs) G(V)G(V) of non-symmetric tunnel junctions between d -wave superconductors with charge-density waves (CDWs) and normal metals were calculated. The dependences G(V)G(V) were shown to have a V-like form at small voltages V and low temperatures, and to be asymmetric at larger V owing to the presence of CDW peak in either of the V-branches. The spatial scatter of the dielectric (CDW) order parameter smears the CDW peak into a hump and induces a peak-dip-hump structure (PDHS) typical of CVCs observed for such junctions. At temperatures larger than the superconducting critical one, the PDHS evolves into a pseudogap depression. The results agree well with the scanning tunneling microscopy data for Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) and YBa sub(2)Cu sub(3)O sub(7- delta ). 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source ScienceDirect Journals (5 years ago - present)
subjects Asymmetry
CHARGE DENSITY
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Conductance
COPPER OXIDE
CUPROUS OXIDE
Electric potential
ELECTRICAL CONDUCTIVITY
Exact sciences and technology
MATHEMATICAL ANALYSIS
Physics
Proximity effects, weak links, tunneling phenomena, and josephson effects, adreev effect, sn and sns junctions
Scanning tunneling microscopy
SUPERCONDUCTIVITY
SUPERCONDUCTORS
Tunneling
YTTRIUM OXIDE
title Charge density waves as the origin of dip-hump structures in the differential tunneling conductance of cuprates: The case of d-wave superconductivity
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