Unadulterated spectral function of low energy quasiparticles: Bi-2212, nodal direction
arXiv:cond-mat/0605100 · doi:10.1103/PhysRevB.74.172509
Abstract
Fitting the momentum distribution photoemission spectra to the Voigt profile appears to be a robust procedure to purify the interaction effects from the experimental resolution. In application to Bi-2212 high-Tc cuprates, the procedure reveals the true scattering rate at low binding energies and temperatures, and, consequently, the true value of the elastic scattering. Reaching the minimal value ~ 16 meV, the elastic scattering does not reveal a systematic dependence on doping level, but is rather sensitive to impurity concentration, and can be explained by the forward scattering on out-of-plane impurities. The inelastic scattering is found to form well-defined quasiparticles with the quadratic and cubic energy dependence of the scattering rate above and below Tc, respectively. The observed energy-temperature asymmetry of the scattering rate is also discussed.
4 revtex pages, 4 figures
References in corpus (6)
- Laser ARPES, the sudden approximation, and quasiparticle-like peaks in Bi2Sr2CaCu2O8+delta
- Self-consistent self-energy analysis of photoemission data
- Bare electron dispersion from photoemission experiments
- Manifestation of the magnetic resonance mode in the nodal quasiparticle lifetime in superconducting cuprates
- Evidence for CuO conducting band splitting in the nodal direction of Bi-2212
- Nodal Quasiparticle Lifetimes in Cuprate Superconductors
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