Speaker
Barbara Mansart
(Ecole Polytechnique Fédérale de Lausanne)
Description
B. Mansart
Laboratory for Ultrafast Microscopy and Electron Scattering, ICMP, Ecole Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
and
Laboratory of Ultrafast Spectroscopy, ISIC, Ecole Polytechnique Fédérale de Lausanne,
CH-1015 Lausanne, Switzerland
J. Lorenzana
ISC-CNR and Dipartimento di Fisica, Università di Roma La Sapienza, P.le Aldo Moro, I-00185 Roma, Italy
M. Scarongella
Laboratory of Ultrafast Spectroscopy, ISIC, Ecole Polytechnique Fédérale de Lausanne,
CH-1015 Lausanne, Switzerland
M. Chergui
Laboratory of Ultrafast Spectroscopy, ISIC, Ecole Polytechnique Fédérale de Lausanne,
CH-1015 Lausanne, Switzerland
F. Carbone
Laboratory for Ultrafast Microscopy and Electron Scattering, ICMP, Ecole Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
Despite their obvious physical difference, from a mathematical (or purely formal) point of view, magnetism and superconductivity are closely linked phenomena. Coherent charge and pairing fluctuations can be described in terms of precession of pseudospins operators, first introduced by Anderson, and behaving as spin-1/2 operators [1].
In our experiment, a polarized ultrafast laser pulse excites the superconductor through the Impulsive Stimulated Raman Scattering (ISRS) effect [2]. The coherent oscillations of the Cooper pairs condensate are detected via delayed supercontinuum pulses and enable a new technique, Coherent Charge Fluctuation Spectroscopy (CCFS), to distinguish the electronic excitations that couple to the superconducting quasiparticles [3].
This is of pivotal importance for cuprates, as the applicability of conventional pairing theories [4], based on retarded interactions between electrons mediated by low energy glue bosons, has been doubted and a completely different framework has been proposed involving non-retarded interactions associated with high-energy electronic scales [5]. We found that the superconducting condensate oscillations resonate at the typical scale of Mott physics (2.6 eV), implying a substantial contribution of non-retarded interactions to the pairing, as in unconventional (non Migdal-Eliashberg) theories.
[1] P.W. Anderson, "Random-Phase Approximation in the theory of superconductivity“, Phys. Rev. 112, 1900 (1958).
[2] R. Merlin, "Generating coherent THz phonons with light pulses", Solid State Comm. 102, 207 (1997).
[3] B. Mansart, J. Lorenzana, M. Scarongella, M. Chergui and F. Carbone, "Direct observation of real-time oscillations of the Cooper-pairs condensate in a high-Tc superconductor", arXiv:1112.0737
[4] G.M. Eliashberg, "Interactions between electrons and lattice vibrations in a superconductor", Soviet Physics JETP 11, 696 (1960).
[5] P.W. Anderson, "The Resonating Valence Bond state in La2CuO4 and Superconductivity", Science 235, 1196 (1987).
Primary author
Barbara Mansart
(Ecole Polytechnique Fédérale de Lausanne)