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Related papers: Quantum Oscillations in the Underdoped Cuprate YBa…

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We study the Fermi surface of metallic, non-magnetic \textit{ortho}-II YBa$_2$Cu$_3$O$_{6.5}$ using three different density-functional-based band-structure techniques (GGA, GGA+U, PSIC). The calculated Fermi surface exhibits no pockets in…

Superconductivity · Physics 2009-11-13 Danilo Puggioni , Alessio Filippetti , Vincenzo Fiorentini

High temperature superconductivity in cuprate superconductors is generally considered to be generated from doping the Mott insulators. The fundamental nature of the doped parent compounds as well as the microscopic origin of electron…

Despite immense efforts, the cuprate Fermi surface (FS) has been unambiguously determined in only two distinct, low-temperature regions of the phase diagram: a large hole-like FS at high doping, and a small electron-like pocket associated…

In the high temperature cuprate superconductors, the pervasiveness of anomalous electronic transport properties suggests that violation of conventional Fermi liquid behavior is closely tied to superconductivity. In other classes of…

Strongly Correlated Electrons · Physics 2012-06-13 N. P. Butch , K. Jin , K. Kirshenbaum , R. L. Greene , J. Paglione

We have measured the extended x-ray absorption-fine-structure (EXAFS) at the Y-K edge of YBa_2Cu_3O_x for x=6.801, 6.947, 6.968, 6.984 at T=20-300 K. Across the underdoped-overdoped transition the Y-Cu2 pairs exhibit harmonic vibrations…

Superconductivity · Physics 2008-02-03 J. Röhler , P. W. Loeffen , S. Müllender , K. Conder , E. Kaldis

A central question in the underdoped cuprates pertains to the nature of the pseudogap ground state. A conventional metallic ground state of the pseudogap region has been argued to host quantum oscillations upon destruction of the…

One of the most striking universal properties of the high-transition-temperature (high-$T_c$) superconductors is that they are all derived from the hole-doping of their insulating antiferromagnetic (AF) parent compounds. From the outset,…

Superconductivity · Physics 2009-10-31 Pengcheng Dai , H. A. Mook , G. Aeppli , S. M. Hayden , F. Dogan

We investigate a chiral d-density wave (CDDW) mean field model Hamiltonian in the momentum space suitable for the hole-doped cuprates, such as YBCO, in the pseudo-gap phase to obtain the Fermi surface(FS)topologies, including the anisotropy…

Superconductivity · Physics 2010-07-29 Partha Goswami , Manju Rani , Avinashi Kapoor

We investigate the properties of cuprate superconductors subject to applied current, using modified Gutzwiller projected d-wave BCS states. The parent states include quasiparticle and quasihole pockets, of variationally determined size,…

Superconductivity · Physics 2010-07-15 Lilach Goren , Ehud Altman

Quantum oscillations are generally studied to resolve the electronic structure of topological insulators. In Cu$_{0.25}$Bi$_2$Se$_3$, the prime candidate of topological superconductors, quantum oscillations are still not observed in…

Strongly Correlated Electrons · Physics 2015-05-13 Ben J. Lawson , Y. S. Hor , Lu Li

Charge density-wave order has been observed in cuprate superconductors whose crystal structure breaks the square symmetry of the CuO2 planes, such as orthorhombic YBa2Cu3Oy (YBCO), but not so far in cuprates that preserve that symmetry,…

We use microprobe Angle-Resolved Photoemission Spectroscopy to study the Fermi surface and band dispersion of the CuO2 planes in the high temperature superconductor, YBa2Cu4O8. We find a strong in-plane asymmetry of the electronic structure…

The currently established electronic phase diagram of cuprates is based on a study of single- and double-layered compounds. These CuO$_2$ planes, however, are directly contacted with dopant layers, thus inevitably disordered with an…

The phase diagram of the cuprate superconductors continues to pose formidable scientific challenges. While these materials are typically viewed as doped Mott insulators, it is well known that they are Fermi liquids at high hole-dopant…

Superconductivity · Physics 2017-08-29 N. Barišić , M. K. Chan , M. J. Veit , C. J. Dorow , Y. Ge , Y. Tang , W. Tabis , G. Yu , X. Zhao , M. Greven

It has been proposed that the pseudogap state of underdoped cuprate superconductors may be due to a transition to a phase which has circulating currents within each unit cell. Here, we use polarized neutron diffraction to search for the…

Superconductivity · Physics 2017-12-18 T. P. Croft , E. Blackburn , J. Kulda , Ruixing Liang , D. A. Bonn , W. N. Hardy , S. M. Hayden

Femtosecond pump probe experiments are reported on quasiparticle relaxation and recombination in YBa2Cu4O8 as a function of temperature and polarization. The data show a 2-component relaxation similar to YBa2Cu3O7-\delta, one component…

Superconductivity · Physics 2008-11-19 D. Dvorsek , V. V. Kabanov , J. Demsar , S. M. Kazakov J. Karpinski , D. Mihailovic

We report scanning Hall probe microscopy of highly underdoped superconducting YBa_2Cu_3O_{6+x} with T_c ranging from 5 to 15 K which showed distinct flux bundles with less than one superconducting flux quantum (Phi_0) through the sample…

Superconductivity · Physics 2009-09-29 J. W. Guikema , Hendrik Bluhm , D. A. Bonn , Ruixing Liang , W. N. Hardy , K. A. Moler

We show that in quasi-two-dimensional $d$-wave superconductors Van Hove singularities close to the Fermi surface lead to novel magnetic quasi-particle excitations. We calculate the temperature and doping dependence of dynamical magnetic…

Condensed Matter · Physics 2009-10-28 G. Blumberg , Branko P. Stojkovic , M. V. Klein

We explore the electronic structure in the heavily overdoped regime of the single layer cuprate superconductor Bi1.74Pb0.38Sr1.88CuO6+delta. We found that the nodal quasiparticle behavior is dominated mostly by phonons, while the antinodal…

We report measurements of the temperature dependent components of the magnetic penetration depth {\lambda}(T) in single crystal samples of YBa_2Cu_4O_8 using a radio frequency tunnel diode oscillator technique. We observe a downturn in…

Superconductivity · Physics 2010-10-22 A. Serafin , J. D. Fletcher , S. Adachi , N. E. Hussey , A. Carrington