Scanning tunnelling microscopy imaging of symmetry-breaking structural distortion in the bismuth-based cuprate superconductors.
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I. Zeljkovic | T. Kondo | Zhijun Xu | J. Wen | H. Ikuta | E. Hudson | G. Gu | J. Hoffman | M. Zech | T. Williams | M. Boyer | Kamalesh Chatterjee | W. D. Wise | Adam Pivonka | E. Main | Y. Yin | T. Takeuchi
[1] J. Hoffman. Spectroscopic scanning tunneling microscopy insights into Fe-based superconductors , 2011, 1201.1380.
[2] J. Orenstein,et al. Point group sensitive probes of the pseudogap electronic structure in Bi2212 , 2011 .
[3] J. Orenstein,et al. From a Single-Band Metal to a High-Temperature Superconductor via Two Thermal Phase Transitions , 2011, Science.
[4] A. Damascelli,et al. Structural origin of apparent Fermi surface pockets in angle-resolved photoemission of Bi₂Sr(2-x)La(x)CuO(6+δ). , 2010, Physical review letters.
[5] G. Gu,et al. Fluctuating stripes at the onset of the pseudogap in the high-Tc superconductor Bi2Sr2CaCu2O8+x , 2010, Nature.
[6] J. Sethna,et al. Intra-unit-cell electronic nematicity of the high-Tc copper-oxide pseudogap states , 2010, Nature.
[7] P. Phillips. Colloquium: Identifying the propagating charge modes in doped Mott insulators , 2010, 1001.5270.
[8] Z. Hussain,et al. Particle-Hole Symmetry Breaking in the Pseudogap State of Bi2201 , 2009, 0911.0197.
[9] S. A. Grigera,et al. Heavy d-electron quasiparticle interference and real-space electronic structure of Sr3Ru2O7 , 2009, 0911.2913.
[10] T. Kondo,et al. Competition between the pseudogap and superconductivity in the high-Tc copper oxides , 2009, Nature.
[11] T. Kondo,et al. Imaging nanoscale Fermi-surface variations in an inhomogeneous superconductor , 2008, 0811.1585.
[12] T. Kondo,et al. Charge-density-wave origin of cuprate checkerboard visualized by scanning tunnelling microscopy , 2008, 0806.0203.
[13] P. Hirschfeld,et al. Imaging the impact on cuprate superconductivity of varying the interatomic distances within individual crystal unit cells , 2008, Proceedings of the National Academy of Sciences of the United States of America.
[14] T. Kondo,et al. Imaging the two gaps of the high-temperature superconductor Bi 2 Sr 2 CuO 6+ x , 2007, 0705.1731.
[15] Dung-Hai Lee,et al. Checkerboard charge density wave and pseudogap of high- T c cuprate , 2006, cond-mat/0606392.
[16] M. Lindroos,et al. Experimental proof of a structural origin for the shadow fermi surface of Bi2Sr2CaCu2O8+delta. , 2006, Physical review letters.
[17] H. Eisaki,et al. Coincidence of checkerboard charge order and antinodal state decoherence in strongly underdoped superconducting Bi2Sr2CaCu2O8 + delta). , 2005, Physical review letters.
[18] G. Kotliar,et al. Pseudogap induced by short-range spin correlations in a doped Mott insulator , 2005, cond-mat/0502565.
[19] R. Gladyshevskii,et al. Structural origin of the low superconducting anisotropy of Bi 1.7 Pb 0.4 Sr 2 Ca 0.9 Cu 2 O 8 crystals , 2004 .
[20] A. Yazdani,et al. Local Ordering in the Pseudogap State of the High-Tc Superconductor Bi2Sr2CaCu2O8+δ , 2004, Science.
[21] H. Eisaki,et al. Coexistence of periodic modulation of quasiparticle states and superconductivity in Bi2Sr2CaCu2O8+δ , 2003, Proceedings of the National Academy of Sciences of the United States of America.
[22] C. Varma,et al. Spontaneous breaking of time-reversal symmetry in the pseudogap state of a high-Tc superconductor , 2002, Nature.
[23] Berkeley,et al. A Four Unit Cell Periodic Pattern of Quasi-Particle States Surrounding Vortex Cores in Bi2Sr2CaCu2O8+δ , 2002, Science.
[24] R. Laughlin,et al. Hidden order in the cuprates , 2000, cond-mat/0005443.
[25] T. Timusk,et al. The pseudogap in high-temperature superconductors: an experimental survey , 1999, cond-mat/9905219.
[26] S. Yoshikado,et al. Detailed structure of a Pb-doped Bi 2 Sr 2 CuO 6 superconductor , 1998 .
[27] V. J. Emery,et al. Electronic liquid-crystal phases of a doped Mott insulator , 1997, Nature.
[28] C. Varma. Non-Fermi-liquid states and pairing instability of a general model of copper oxide metals , 1996, cond-mat/9607105.
[29] J. Hejtmánek,et al. Structural modulation, oxygen content and transport properties in Bi2.13Sr1.87CuO6+y and Bi2.05Sr1.54La0.41CuO6+y superconductors , 1994 .
[30] A. Migliori,et al. Structural modulation and superconducting properties in (Bi, Pb) 2Sr2 (Y, Ca) Cu2Oz , 1992 .
[31] R. Buckley,et al. General trends in oxygen stoichiometry effects on Tc in Bi and Tl superconductors , 1991 .
[32] Lee,et al. X-ray analysis of the incommensurate modulation in the 2:2:1:2 Bi-Sr-Ca-Cu-O superconductor including the oxygen atoms. , 1990, Physical review. B, Condensed matter.
[33] O. Gunnarsson,et al. Charged magnetic domain lines and the magnetism of high-Tc oxides. , 1989, Physical review. B, Condensed matter.
[34] Zhongxian Zhao,et al. Direct observation of antiphase domains in Bi2Sr2CaCu2O8 by transmission electron microscopy , 1989 .
[35] P Coppens,et al. The Incommensurate Modulation of the 2212 Bi-Sr-Ca-Cu-O Superconductor , 1988, Science.
[36] Morrissey,et al. Structures of the superconducting oxides Tl2Ba2CuO6 and Bi2Sr2CuO6. , 1988, Physical review. B, Condensed matter.
[37] C. Torardi,et al. A New High-Temperature Superconductor: Bi2Sr3-x Cax Cu2O8+y , 1988, Science.
[38] T. Williams. Nanoscale Electronic Structure of Cuprate Superconductors Investigated with Scanning Tunneling Spectroscopy , 2011 .
[39] A. Karki,et al. Nanoscale chemical phase separation in FeTe0.55Se0.45 as seen via scanning tunneling spectroscopy , 2011 .
[40] G. McIntyre,et al. Refinement of the incommensurate structure of high quality Bi-2212 single crystals from a neutron diffraction study , 1998 .