Temperature-Dependent Ellipsometry Measurements of Partial Coulomb Energy in Superconducting Cuprates

• Published in: Physical review. X Vol. 6; no. 3; p. 031027
• Main Authors: Levallois, J., Tran, M. K., Pouliot, D., Presura, C. N., Greene, L. H., Eckstein, J. N., Uccelli, J., Giannini, E., Gu, G. D., Leggett, A. J., van der Marel, D.
• Format: Journal Article
• Language: English
• Published: College Park American Physical Society 24-08-2016
• Subjects: Bismuth strontium calcium copper oxide; Condensates; CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; Conduction cooling; Conduction electrons; Conduction heating; Cooper pairs; Cuprates; Doping; Ellipsometry; Energy; High temperature; Momentum; Phase transitions; Questions; Single crystals; Superconductivity; Superconductors; Temperature dependence; Transition temperature
• ISSN: 2160-3308; 2160-3308
• DOI: 10.1103/PhysRevX.6.031027

We performed an experimental study of the temperature and doping dependence of the energy-loss function of the bilayer and trilayer bismuth cuprates family. The primary aim is to obtain information on the energy stored in the Coulomb interaction between the conduction electrons, on the temperature dependence thereof, and on the change of Coulomb interaction when Cooper pairs are formed. We performed temperature-dependent ellipsometry measurements on several Bi2Sr2CaCu2O8−x single crystals: underdoped with Tc=60 , 70, and 83 K; optimally doped with Tc=91K ; overdoped with Tc=84 , 81, 70, and 58 K; as well as optimally doped Bi2Sr2Ca2Cu3O10+x with Tc=110K . Our first observation is that, as the temperature drops through Tc , the loss function in the range up to 2 eV displays a change of temperature dependence as compared to the temperature dependence in the normal state. This effect at—or close to—Tc depends strongly on doping, with a sign change for weak overdoping. The size of the observed change in Coulomb energy, using an extrapolation with reasonable assumptions about its q dependence, is about the same size as the condensation energy that has been measured in these compounds. Our results therefore lend support to the notion that the Coulomb energy is an important factor for stabilizing the superconducting phase. Because of the restriction to small momentum, our observations do not exclude a possible significant contribution to the condensation energy of the Coulomb energy associated with the region of q around (π,π) .