cmp-seminars

On the Electron Pairing Mechanism of Copper-Oxide High Temperature Superconductivity

18 Nov 2021
Seminars and colloquia
Time
Venue
First Floor Audrey Wood Meeting Room
Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford, OX1 3PU
Speaker(s)

Prof Seamus Davis, University of Oxford

https://zoom.us/j/93960665077

Seminar series
CMP seminar
Knowledge of physics?
Yes, knowledge of physics required
For more information contact

Maud Schmitt

The elementary CuO2 plane sustaining cuprate high-temperature superconductivity occurs typically at the base of a periodic array of edge-sharing CuO5 pyramids (Fig 1a). Virtual transitions of electrons between adjacent planar Cu and O atoms, occurring at a rate t/ and across the charge-transfer energy gap E, generate 'superexchange' spin-spin interactions of energy J≈4t4/E3 in an antiferromagnetic correlated-insulator state1. Hole doping the CuO2 plane disrupts this magnetic order while perhaps retaining superexchange interactions, thus motivating a hypothesis of spin-singlet electron-pair formation at energy scale J as the mechanism of high-temperature superconductivity. Although the response of the superconductor's electron-pair wavefunction Ψ≡<cc> to alterations in E should provide a direct test of such hypotheses, measurements have proven impracticable. Focus has turned instead to the distance δ between each Cu atom and the O atom at the apex of its CuO5 pyramid. Varying δ should alter the Coulomb potential at the planar Cu and O atoms, modifying E and thus J, and thereby controlling Ψ in a predictable manner. Here we implement atomic-scale imaging of E and Ψ, both as a function of the periodic modulation in δ that occurs naturally in Bi2Sr2CaCu2O8+x. We demonstrate that the responses of E and Ψ to varying δ, and crucially those of Ψ to the varying E, conform to theoretical predictions. These data provide direct atomic-scale verification that charge-transfer superexchange is key to the electron-pairing mechanism in the hole-doped cuprate superconductor Bi2Sr2CaCu2O8+x.