2006 APS March Meeting
Monday–Friday, March 13–17, 2006;
Baltimore, MD
Session N23: Focus Session: MAG.THY III: Oxides and Phase Transitions
8:00 AM–10:48 AM,
Wednesday, March 15, 2006
Baltimore Convention Center
Room: 320
Sponsoring
Units:
GMAG DMP DCOMP
Chair: Bruce Harmon, Ames Laboratory
Abstract ID: BAPS.2006.MAR.N23.4
Abstract: N23.00004 : Towards material-specific simulations of high-temperature superconducting cuprates*
8:36 AM–9:12 AM
Preview Abstract
Abstract
Author:
Thomas Schulthess
(Oak Ridge National Laboratory)
Simulations of high-temperature superconducting (HTSC) cuprates
have typically fallen into two categories: (1) studies of generic
models such as the two-dimensional (2D) Hubbard model, that are
believed to capture the essential physics necessary to describe
the superconducting state, and, (2) first principles electronic
structure calculations that are based on the local density
approximation (LDA) to density functional theory (DFT) and lead
to materials specific models. With advent of massibely parallel
vector supercomputers, such as the Cray X1E at ORNL, and cluster
algorithms such as the Dynamical Cluster Approximation (DCA), it
is now possible to systematically solve the 2D Hubbard model with
Quantum Monte Carol (QMC) simulations and to establish that the
model indeed describes $d$-wave superconductivity [1].
Furthermore, studies of a multi-band model with input parameters
generated from LDA calculations demonstrate that the existence of
a superconducting transition is very sensitive to the underlying
band structure [2]. Application of the LDA to transition metal
oxides is, however, hampered by spurious self-interactions that
particularly affects localized orbitals. Here we apply the
self-interaction corrected local spin-density method (SIC-LSD) to
describe the electronic structure of the cuprates. It was
recently applied with success to generate input parameters for
simple models of Mn doped III-V semiconductors [3] and is known
to properly describe the antiferromagnetic insulating ground
state of the parent compounds of the HTSC cuprates. We will
discus the models for HTSC cuprates derived from the SIC-LSD
study and how the differences to the well-known LDA results
impact the QMC-DCA simulations of the magnetic and
superconducting properties.
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[1] T. A. Maier, M. Jarrell, T. C. Schulthess, P. R. C. Kent, and
J. B. White, Phys. Rev. Lett. 95, 237001 (2005).
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[2] P. Kent, A. Macridin, M. Jarrell, T. Schulthess, O. Andersen,
T. Dasgupta, and O. Jepsen, Bulletin of the American Physical
Sosciety 50, 1057 (2005).
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[3] T. C. Schulthess, W. Temmerman, Z. Szotek, W. H. Butler, and
G. M. Stocks, Nature Materials 4, 838 (2005).
*Work enabled by computational resources of the Center of Computational Sciences at Oak Ridge National Laboratory and supported by the Division of Materials Science and Engineering, U. S. Department of Energy.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2006.MAR.N23.4