Observation of a d-wave gap in electron-doped Sr2IrO4

[1]  Y. J. Yan,et al.  Signature of high temperature superconductivity in electron doped Sr2IrO4 , 2015, 1506.06557.

[2]  S. M. Walker,et al.  Collapse of the Mott Gap and Emergence of a Nodal Liquid in Lightly Doped Sr(2)IrO(4). , 2015, Physical review letters.

[3]  B. J. Kim,et al.  Direct evidence for dominant bond-directional interactions in a honeycomb lattice iridate Na2IrO3 , 2015, Nature Physics.

[4]  I. Vobornik,et al.  Transfer of spectral weight across the gap of Sr 2 IrO 4 induced by La doping , 2015, 1503.08120.

[5]  M. R. Norman,et al.  From quantum matter to high-temperature superconductivity in copper oxides , 2015, Nature.

[6]  John M. Tranquada,et al.  Colloquium : Theory of intertwined orders in high temperature superconductors , 2014, 1407.4480.

[7]  T. Devereaux,et al.  Energy gaps in high-transition-temperature cuprate superconductors , 2014, Nature Physics.

[8]  A. Bostwick,et al.  Hallmarks of the Mott-Metal Crossover in the Hole Doped J=1/2 Mott insulator Sr2IrO4 , 2014, 1406.4978.

[9]  A. Bostwick,et al.  Fermi arcs in a doped pseudospin-1/2 Heisenberg antiferromagnet , 2014, Science.

[10]  Yong Baek Kim,et al.  Odd-parity triplet superconducting phase in multiorbital materials with a strong spin-orbit coupling: application to doped Sr₂IrO₄. , 2014, Physical review letters.

[11]  Zhi-Xun Shen,et al.  Direct observation of the transition from indirect to direct bandgap in atomically thin epitaxial MoSe2. , 2014, Nature nanotechnology.

[12]  S. Yunoki,et al.  Monte Carlo study of an unconventional superconducting phase in iridium oxide J(eff)=1/2 Mott insulators induced by carrier doping. , 2012, Physical review letters.

[13]  B. J. Kim,et al.  Large spin-wave energy gap in the bilayer iridate Sr3Ir2O7: evidence for enhanced dipolar interactions near the mott metal-insulator transition. , 2012, Physical review letters.

[14]  Jungho Kim,et al.  Magnetic excitation spectra of Sr2IrO4 probed by resonant inelastic x-ray scattering: establishing links to cuprate superconductors. , 2012, Physical review letters.

[15]  B. J. Kim,et al.  Two-dimensional Heisenberg behavior of J(eff)=1/2 isospins in the paramagnetic state of the spin-orbital Mott insulator Sr2IrO4. , 2012, Physical review letters.

[16]  A. Fujimori,et al.  Pseudogap, Superconducting Gap, and Fermi Arc in High-Tc Cuprates Revealed by Angle-Resolved Photoemission Spectroscopy , 2012, 1203.0600.

[17]  K. Held,et al.  Pseudogap of metallic layered nickelate R(2-x)Sr(x)NiO4 (R = Nd, Eu) crystals measured using angle-resolved photoemission spectroscopy. , 2010, Physical review letters.

[18]  T. Senthil,et al.  Twisted Hubbard model for Sr2IrO4: magnetism and possible high temperature superconductivity. , 2010, Physical review letters.

[19]  M. Randeria,et al.  Observation of a d -wave nodal liquid in highly underdoped Bi 2 Sr 2 CaCu 2 O 8+ δ , 2009, 0910.1648.

[20]  T. Ozaki,et al.  Anisotropic exchange interactions of spin-orbit-integrated states in Sr2IrO4 , 2008, 0808.3491.

[21]  S. Sakai,et al.  Phase-Sensitive Observation of a Spin-Orbital Mott State in Sr2IrO4 , 2009, Science.

[22]  G. Jackeli,et al.  Mott insulators in the strong spin-orbit coupling limit: from Heisenberg to a quantum compass and Kitaev models. , 2008, Physical review letters.

[23]  A. Bostwick,et al.  In situ doping control of the surface of high-temperature superconductors , 2008 .

[24]  Jaejun Yu,et al.  Novel Jeff=1/2 Mott state induced by relativistic spin-orbit coupling in Sr2IrO4. , 2008, Physical review letters.

[25]  Z. Hussain,et al.  Abrupt onset of a second energy gap at the superconducting transition of underdoped Bi2212 , 2007, Nature.

[26]  G. Gu,et al.  The Ground State of the Pseudogap in Cuprate Superconductors , 2006, Science.

[27]  T. Ohta,et al.  Controlling the Electronic Structure of Bilayer Graphene , 2006, Science.

[28]  Z. Hussain,et al.  Nodal quasiparticle in pseudogapped colossal magnetoresistive manganites , 2005, Nature.

[29]  X. Chaud,et al.  Magnetic order in the pseudogap phase of high-Tc superconductors. , 2005, Physical review letters.

[30]  C. Varma.  Theory of the pseudogap state of the cuprates , 2005, cond-mat/0507214.

[31]  M. Crawford,et al.  Anomalous magnetic and transport behavior in the magnetic insulator Sr 3 Ir 2 O 7 , 2002 .

[32]  J. Eckstein,et al.  Signature of superfluid density in the single-particle excitation spectrum of Bi2Sr2CaCu2O8+δ , 2000, cond-mat/0009306.

[33]  R. Laughlin,et al.  Hidden order in the cuprates , 2000, cond-mat/0005443.

[34]  M. R. Norman,et al.  Phenomenology of the low-energy spectral function in high-T c superconductors , 1998 .

[35]  M. Fisher,et al.  Nodal Liquid Theory of the Pseudo-Gap Phase of High-Tc Superconductors , 1998, cond-mat/9803086.

[36]  Wang,et al.  Structural and magnetic studies of Sr2IrO4. , 1994, Physical review. B, Condensed matter.

[37]  Affleck,et al.  Large-n limit of the Hubbard-Heisenberg model. , 1989, Physical review. B, Condensed matter.

[38]  Brink,et al.  Evidence for Enhanced Dipolar Interactions Near the Mott Metal-Insulator Transition , 2014 .

[39]  Z. Hussain,et al.  Abrupt Onset of Second Energy Gap at Superconducting Transition of Underdoped Bi 2212 , 2008 .

[40]  Shen,et al.  Signature of superfluid density in the single-particle excitation spectrum of Bi(2)Sr(2)CaCu(2)O(8+delta) , 2000, Science.