APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session Z2: Pseudogap in High Tc Cuprates
11:15 AM–2:15 PM,
Friday, March 25, 2011
Room: Ballroom A2
Sponsoring
Unit:
DCMP
Chair: Martin Greven, University of Minnesota
Abstract ID: BAPS.2011.MAR.Z2.2
Abstract: Z2.00002 : Novel magnetic excitations in a model cuprate high-$T_{c}$ superconductor*
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Yuan Li
(Max Planck Institute for Solid State Research, Germany)
Magnetic fluctuations might be essential to the mechanism of
high-temperature superconductivity in the cuprates. For a long
time, such fluctuations have been theoretically regarded as
arising from the antiferromagnetic correlations within the
copper-oxygen layers, and experimental studies of magnetic
excitation spectrum have mainly been carried out near the
corresponding wave vector (1/2,~1/2). Following neutron
diffraction experiments which demonstrated the universal
existence of a ``$q$~=~0 antiferromagnetic order'' in the
pseudogap phase of three different
cuprates [1-3], our recent inelastic neutron scattering
experiments on the
model compound HgBa$_{2}$CuO$_{4+\delta }$ (Hg1201) revealed the
existence
of unusual magnetic excitations that weakly disperse throughout
the entire
Brillouin zone [4,5]. Like the $q$~=~0 antiferromagnetic order,
the new
excitations are observed in the pseudogap phase and therefore
appear to be
associated with the order. The excitations possess very large
spectral
weights at well-defined characteristic energies that are
comparable to the
resonance energy [6] and to those of electron-boson-coupling
features
observed in a wide range of cuprates, highlighting their possible
influence
on the electronic structure. These findings demonstrate that the
pseudogap
state is a distinct phase of matter rather than a mere crossover.
They
furthermore cast doubt on the presumed predominant importance of
the wave
vector (1/2,~1/2) in the magnetic excitation spectrum, and have
the profound
implication that a single-band description of the cuprates is
insufficient.
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[1] B. Fauque \textit{et al.}, \textit{Phys. Rev. Lett.}
\textbf{96}, 197001 (2006).
\\[0pt]
[2] Yuan Li \textit{et al.}, \textit{Nature} \textbf{455}, 372
(2008).
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[3] V. Baledent \textit{et al.}, \textit{Phys. Rev. Lett.}
\textbf{105}, 027004 (2010).
\\[0pt]
[4] Yuan Li \textit{et al.}, \textit{Nature} \textbf{468}, 283
(2010).
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[5] Yuan Li \textit{et al.}, unpublished.
\\[0pt]
[6] G. Yu \textit{et al.}, \textit{Phys. Rev. B} \textbf{81},
064518 (2010).
*Project was funded by DOE and NSF grants. The author achnowledges the Alexander von Humboldt Foundation.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.Z2.2