2008 APS March Meeting
Volume 53, Number 2
Monday–Friday, March 10–14, 2008;
New Orleans, Louisiana
Session Y31: Focus Session: Sodium Cobaltites
11:15 AM–2:03 PM,
Friday, March 14, 2008
Morial Convention Center
Room: 223
Sponsoring
Units:
DMP GMAG
Chair: David Singh, Oak Ridge National Laboratory
Abstract ID: BAPS.2008.MAR.Y31.1
Abstract: Y31.00001 : Charge order and anomalous magnetism in the Na cobaltates
11:15 AM–11:51 AM
Preview Abstract
Abstract
Author:
Henri Alloul
(Physique des Solides, CNRS UMR 8502, univ. Paris-Sud, 91405 ORSAY)
The layered Na cobaltates have some analogies with the
cuprates~as 2D
conductivity occurs in the CoO$_{2}$ planes and doping can be
modified by
changing the Na content. Also ordered magnetic phases have been
evidenced,
but unexpectedly for large values of $x$ for which one would
expect a hole
doping of the band insulator NaCoO$_{2}$. Indeed, in the high
crystal field
on the Co sites in these compounds, an ionic picture for the Co
states would
correspond to low spin configurations Co$^{3+}$, S=0 or
Co$^{4+}$, S=1/2.
We shall present SQUID and $^{23}$Na and $^{59}$Co NMR data [1]
taken on samples synthetized and characterized by X ray
cristallography in
LLB, Saclay. We evidence that the Co charge is uniform for
$x$=0.35 as in the
hydrated superconducting phase. For high Na contents the samples
are found
to display ordered Na structures or mixtures of those, with
different $x$
values. In pure phases isolated for specific $x$ values, we
evidence a charge
disproportionation into non magnetic Co$^{3+}$ and more magnetic
Co sites
with an average charge of about Co$^{3.5+}$, except for
$x$=0.5 [2]. This
hole delocalization and charge order occur both for paramagnetic
and AF phases [3]. NMR investigations of the dynamic
susceptibilities allow us to characterize the nature of the in
plane electronic correlations in most parts of the phase diagram.
Contrary to the case of most cuprates for which dopant disorder
is quite influential, the hole doping achieved in cobaltate
samples is associated with the insertion of well ordered Na
planar structures. They have to be taken into account to explain
theoretically the metallicity, the magnetic properties and their
evolution with doping.
\newline
[1] \textit{I. Mukhamedchine, H. Alloul, G. Collin et N.
Blanchard, Phys. Rev. Letters, }\textbf{\textit{ 94}}\textit{,
247602 (2005). }
\newline
[2] http://arxiv.org/find/cond-mat/1/au:+Bobroff\_J/0/1/0/all/0/1,
J. Bobroff;
http://arxiv.org/find/cond-mat/1/au:+Lang\_G/0/1/0/all/0/1, G.
Lang;
http://arxiv.org/find/cond-mat/1/au:+Alloul\_H/0/1/0/all/0/1, H.
Alloul;
http://arxiv.org/find/cond-mat/1/au:+Blanchard\_N/0/1/0/all/0/1,
N. Blanchard and
http://arxiv.org/find/cond-mat/1/au:+Collin\_G/0/1/0/all/0/1, G.
Collin, \textit{Phys. Rev. Letters \textbf{\textit{96}},
107201 (2006) .}
\newline
[3] \textit{I. Mukhamedchine, H. Alloul, G. Collin et N.
Blanchard, condmat /0703561. }
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2008.MAR.Y31.1