2007 APS March Meeting
Volume 52, Number 1
Monday–Friday, March 5–9, 2007;
Denver, Colorado
Session P4: Magnetic Bose-Einstein Condensation
11:15 AM–2:15 PM,
Wednesday, March 7, 2007
Colorado Convention Center
Room: Korbel 2B-3B
Sponsoring
Unit:
GMAG
Chair: Stephen Hill, University of Florida
Abstract ID: BAPS.2007.MAR.P4.5
Abstract: P4.00005 : Quasiparticle condensation and breakdown in a quantum spin liquid*
1:39 PM–2:15 PM
Preview Abstract
Abstract
Author:
Matthew Stone
(Oak Ridge National Laboratory)
Piperazinium hexachlorodicuprate (PHCC) is a frustrated bilayer
antiferromagnet with a disordered quantum spin-liquid (QSL)
ground state at zero field [1] and a diverse magnetic field
versus temperature phase diagram which includes two field-
induced quantum critical points [2]. The spin excitations in
PHCC have a spectral gap of $\Delta \approx 1$~meV above which
they follow a nearly 2D-isotropic dispersion with a bandwidth
slightly larger than $\Delta$. Field dependent neutron
scattering and thermodynamic measurements reveal a lower
critical field, $H_{c1}=7.5$~T, separating the QSL phase from a
three dimensional spin-ordered state and an upper critical
field, $H_{c2}=37$~T, marking the onset of a saturated
ferromagnetic phase. The two-dimensional antiferromagnet
supports a field induced long range ordered phase well described
as a Bose-Einstein condensate (BEC) embedded within a gapless
quasi-two-dimensional paramagnetic regime. Inelastic neutron
scattering experiments also reveal a peculiar type of
hybridization of magnetic excitations in PHCC with their two-
particle continuum [3], similar to the post-roton regime in
superfluid helium. The excitations at this point become
broadened and diffuse, no longer describable as quasiparticles.
Although such effects are expected to be strongest in one-
dimensional systems with gapped spectra [4], such as Haldane
chains, direct observation therein is difficult due to a weak
scattering structure factor in the vicinity of the quasiparticle
breakdown point [5,6]. The dimer-dominated magnetism in PHCC, on
the other hand, is favorable for investigating changes in
quasiparticle spectra in the vicinity of their breakdown point.
Our results have implications for a variety of condensed
matter systems, in particular for other QSLs, where spin
excitations have a bandwidth greater than the gap energy.
\newline
[1] M. B. Stone, {\it et al}. Phys. Rev. B {\bf 64}, 144405
(2001).\newline
[2] M. B. Stone, {\it et al}. Phys. Rev. Lett. {\bf 96}, 257203
(2006).\newline
[3] M. B. Stone, {\it et al}. Nature, {\bf 440}, 187 (2006).\newline
[4] T. Giamarchi, Quantum Physics in One Dimension, Oxford
University Press (2005).\newline
[5] S. Ma, {\it et al}. Phys. Rev. Lett. {\bf 69}, 3571
(1992).\newline
[6] I. A. Zaliznyak, {\it et al}. Phys. Rev. Lett. {\bf 87},
017202 (2001).
*Work performed in collaboration with I. Zaliznyak, D. H. Reich, C. L. Broholm, O. Tchernyshyov, P. Vorderwisch, T. Hong, and N. Harrison
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2007.MAR.P4.5