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Electronic Raman Spectroscopy in a Nut Shell (I). Yu He SC Meeting Oct 10, 2013. Raman and History Experimental Setup Geometry in Raman Position Raman among other Techniques Raman in Superconducting Materials Mode coupling SC Gap. Main conclusion figures.
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Electronic Raman Spectroscopy in a Nut Shell (I) Yu He SC Meeting Oct 10, 2013 • Raman and History • Experimental Setup • Geometry in Raman • Position Raman among other Techniques • Raman in Superconducting Materials • Mode coupling • SC Gap Main conclusion figures
Electronic Raman Spectroscopy in a Nut Shell (I) • Raman and History • Experimental Setup • Geometry in Raman • Position Raman among other Techniques • Raman in Superconducting Materials • Mode coupling • SC Gap Main conclusion figures
From Molecules to Solid Molecules (gas and liquid) Resonant Inelastic X-ray Scattering Solid (electronic) Electronic Raman Spectroscopy
Electronic Raman Spectroscopy in a Nut Shell (I) Yu He SC Meeting Oct 10, 2013 • Raman and History • Experimental Setup • Geometry in Raman • Position Raman among other Techniques • Raman in Superconducting Materials • Mode coupling • SC Gap Main conclusion figures
Backscattering Raman electro-optic modulator (EOM) Two-gap dichotomy is NOT universal (in UD regime)
Electronic Raman Spectroscopy in a Nut Shell (I) Yu He SC Meeting Oct 10, 2013 • Raman and History • Experimental Setup • Geometry in Raman • Position Raman among other Techniques • Raman in Superconducting Materials • Mode coupling • SC Gap Main conclusion figures
Single Particle vs Two Particles e-ph: Migdal Coulomb: FL, MFL e-magnon
Electronic Raman Spectroscopy in a Nut Shell (I) Yu He SC Meeting Oct 10, 2013 • Raman and History • Experimental Setup • Geometry in Raman • Position Raman among other Techniques • Raman in (Superconducting) Materials • Mode coupling • SC Gap Main conclusion figures
Start from single metal? • Not so easy! • Strong screening – small interaction volume • Parabolic dispersion and spherical FS – further reduce cross section
‘HighTc’ Convenional SC 1.8K V3Si 40K 1.8K 1.8K Nb3Sn
Competition and Mode Coupling Tc ~ 7.2K, Tcdw ~33K, Hc2 ~42kG
Highc SC No dichotomy when QP is well defined across all fermi surface Dichotomy appears when QP disappears from N to AN
Highc SC Bi2212
Highc SC M. Le Tacon et al., Nat. Phys. 2, 537 (2006)
Highc SC 0.15 0.22 0.20 Bi2212
Highc SC Two magnonexcitations
FT- Raman RIXS