Interaction of phonons with intraband electronic excitations and crystal field transitions in Raman spectra of (Nd,Eu,Gd)Ba2Cu3Oy crystals

[1]  M. L. Tacon,et al.  Lattice dynamical signature of charge density wave formation in underdoped YBa 2 Cu 3 O 6 + x , 2013, 1312.1082.

[2]  Yuri S. Kivshar,et al.  Fano Resonances in Nanoscale Structures , 2010 .

[3]  M. Cardona,et al.  Electronic and phononic Raman scattering in detwinned YBa2Cu3O6.95 and Y0.85Ca0.15Ba2Cu3O6.95: s-wave admixture to the dx2-y2-wave order parameter , 2009, 0907.4587.

[4]  N. Sakai,et al.  Record flux pinning in melt-textured NEG-123 doped by Mo and Nb nanoparticles , 2008 .

[5]  T. Devereaux,et al.  Inelastic light scattering from correlated electrons , 2006, cond-mat/0607554.

[6]  S. Reich,et al.  Raman spectroscopy with UV excitation on untwinned single crystals of YBa2Cu3O7–δ , 2004 .

[7]  N. Sakai,et al.  New type of vortex pinning structure effective at very high magnetic fields. , 2002, Physical review letters.

[8]  A. Yamanaka,et al.  Zn doping effect on the superconducting gap in YBa2Cu3O7-Φ: Raman study , 2001 .

[9]  M. Kakihana,et al.  Raman active modes in Nd2BaCu3Oz compound , 2000 .

[10]  A. Yamanaka,et al.  Superconductivity-induced effects on phononic and electronic Raman scattering in twin-free YBa 2 Cu 3 O 7-x single crystals , 2000 .

[11]  H. Berger,et al.  Carrier relaxation, pseudogap, and superconducting gap in high-Tc cuprates: A Raman scattering study , 1999, cond-mat/9908272.

[12]  R. Sharma,et al.  Anomalous self-energy effects of the B 1 g phonon in Y 1 − x ( Pr , Ca ) x Ba 2 Cu 3 O 7 films , 1999, cond-mat/9908355.

[13]  M. Cardona,et al.  Raman study of coupled-phonon–crystal-field excitations in Nd 1 + x Ba 2 − x Cu 3 O y single crystals , 1998 .

[14]  M. Cardona,et al.  Anomalous phonon self-energy effects in SmBa_ {2} Cu_ {3} O_ {y}: A Raman study , 1998 .

[15]  T. Wolf,et al.  Peak effect and its evolution from oxygen deficiency in YBa 2 Cu 3 O 7 − δ single crystals , 1998 .

[16]  M. Cardona,et al.  Determination of the phase difference between the Raman tensor elements of the A 1 g -like phonons in SmBa 2 Cu 3 O 7 − δ , 1998 .

[17]  M. Murakami,et al.  Improved superconducting properties of melt-textured Nd123 by additional heat treatment , 1997 .

[18]  M. Cardona,et al.  Growth of (110)-oriented epitaxial RBa2Cu3O7−δ thin films and characterization with Raman spectroscopy , 1997 .

[19]  N. Sakai,et al.  Melt-processed light rare earth element - Ba - Cu - O , 1996 .

[20]  R. Evarestov,et al.  Optical Phonons and Their Role in High‐Tc Superconductivity Mechanism , 1993 .

[21]  Chen,et al.  Oxygen-concentration dependence of the Raman continua in YBa2Cu3Oy single crystals. , 1993, Physical review. B, Condensed matter.

[22]  Klein,et al.  Plane-polarized Raman continuum in the insulating and superconducting layered cuprates. , 1993, Physical review. B, Condensed matter.

[23]  G. Ries,et al.  Time and orientation dependent magnetic measurements and increase of the critical current by fast neutron irradiation of Y1Ba2Cu3O7- deltasingle crystals , 1992 .

[24]  Klein,et al.  Optically induced metastability in untwinned single-domain YBa2Cu3O7. , 1991, Physical review letters.

[25]  Cardona,et al.  Raman study of the coupling of crystal-field excitations to phonons in NdBa2Cu3O7- delta. , 1991, Physical review. B, Condensed matter.

[26]  C. Loong,et al.  Crystal-field properties of f-electron states in RBa2Cu3O7 for R = Ho, Nd and Pr , 1991 .

[27]  G. Roth,et al.  Growth of thick YBa2Cu3O7−x single crystals from Al2O3 crucibles , 1989 .

[28]  R. Feile.  Lattice vibrations in high-Tc superconductors: Optical spectroscopy and lattice dynamics☆ , 1989 .

[29]  Liu,et al.  Untwinned single crystals of YBa2Cu3O7- delta : An optical investigation of the a-b anisotropy. , 1988, Physical review. B, Condensed matter.

[30]  James F. Scott,et al.  Scattering of Light by Crystals , 1998 .