APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session P18: Focus Session: Low D/Frustrated Magnetism - Triangular Lattices
8:00 AM–11:00 AM,
Wednesday, March 23, 2011
Room: D172
Sponsoring
Units:
GMAG DMP
Chair: Bruce Gaulin, McMaster University
Abstract ID: BAPS.2011.MAR.P18.1
Abstract: P18.00001 : Neutron Scattering Studies of the S=1/2 Triangular Lattice Magnets NaNiO$_2$ and LiNiO$_2$
8:00 AM–8:36 AM
Preview Abstract
Abstract
Author:
J. Patrick Clancy
(McMaster University)
NaNiO$_2$ and LiNiO$_2$ are isostructural quantum magnets based
on a stacked triangular lattice in which magnetism arises from
S=1/2 magnetic moments carried by Ni$^{3+}$ ions. Surprisingly,
while these compounds are structurally and electronically very
similar, the magnetic properties they exhibit are dramatically
different. NaNiO$_2$ undergoes a cooperative Jahn-Teller phase
transition at 480K and magnetically orders below T$_N$ $\sim$
23K, adopting a structure which consists of ferromagnetic sheets
of S=1/2 moments stacked in an antiferromagnetic fashion. In
contrast, LiNiO$_2$ undergoes a spin glass transition at T$_g$
$\sim$ 9K and remains disordered down to the lowest measured
temperatures. Understanding the absence of long-range magnetic
order in LiNiO$_2$ is a problem which has attracted considerable
interest for more than twenty five years. Among many potential
explanations, the answer has most notably been attributed to
geometric frustration caused by inherent mixing of the Li and Ni
sublattices, or orbital degeneracy resulting from the lack of a
coherent Jahn-Teller distortion.
In this talk I will describe time-of-flight neutron scattering
measurements performed on polycrystalline samples of NaNiO$_2$
and LiNiO$_2$ using the wide Angular-Range Chopper Spectrometer
(ARCS) at ORNL and the Disk Chopper Spectrometer (DCS) at NIST.
These measurements provide a thorough characterization of the
excitation spectra for these two compounds, probing the inelastic
scattering over energy scales ranging from $\sim$ 0.1 meV to 1.5
eV. In NaNiO$_2$, our measurements reveal two sets of
well-defined spin excitations, which we associate with
ferromagnetic spin waves mediated by in-plane interactions and
antiferromagnetic spin waves mediated by out-of-plane
interactions. In LiNiO$_2$, we observe similar, albeit much
broader, excitations consistent with short-range two-dimensional
magnetic correlations. In the case of NaNiO$_2$, we have
developed a simple linear spin wave theory model to describe
these excitations and extract the relevant magnetic exchange
couplings for this system.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.P18.1