Bulletin of the American Physical Society
APS March Meeting 2018
Volume 63, Number 1
Monday–Friday, March 5–9, 2018; Los Angeles, California
Session V30: Superconductivity: General Theory
2:30 PM–5:30 PM,
Thursday, March 8, 2018
LACC
Room: 406B
Sponsoring
Unit:
DCMP
Chair: Brian Moritz, SLAC National Accelerator Laboratory
Abstract ID: BAPS.2018.MAR.V30.12
Abstract: V30.00012 : Prediction of Universal Peak in Electronic Thermal Conductivity of High Temperature Superconductors via Dipolon Theory
4:42 PM–4:54 PM
Presenter:
Ram Sharma
(Univ of Illinois - Chicago)
Author:
Ram Sharma
(Univ of Illinois - Chicago)
The dipolon
theory [1-4]
has predicted
the two high energy and one low energy
quasiparticle (QP) kinks
besides
a new very low energy kink
in
hIgh $T_C$ superconductors
(HTSCs).
Here we report the prediction of a
universal peak
in electronic thermal conductivity
(ETC)
of
HTSCs.
We find that
the ETC
in HTSCs is due to
the rate of enhancement
with
temperature
of the
QP energy distribution
particularly near
the M point of the Fermi level (high QP density region),
which becomes maximum at the
temperature
$T^{(peak)}$ given by
$x = ln( \frac {x+2}{x-2})$
where
$ x = \Delta (0) /k_BT^{(peak)}$
yielding
$ T^{(peak)} = \Delta (0) /2.40 k_B. $
This peak
is valid for all HTSCs and for all directions
of ETC in the a-b plane and hence is a
universal peak.
For HTSCs where
$\Delta (0) = 1.5k_BT_C $,
we have
$T^{(peak)}
=0.6 T_C$,
in agreement with the experimental results [5]
$T^{peak}_{expt}
/T_C = 0.6 \pm 0.2. $
(1) R. R. Sharma, Phy. Rev. {\bf B 63}, 054506 (2001).
(2) R. R. Sharma, Physica {\bf C 439}, 47 (2006).
(3) R. R. Sharma, Physica {\bf C 468}, 190 (2008).
(4) R. R. Sharma, "Dipolon Theory of Kink Structure
...", in "Superconducting ...", Ed. K. N. Courtlandt,
P. 81-100, Nova Sc, Pub., Inc., New York, 2009.
(5) C. Uher, in "Phys. Propertie ...",
Ed. D. M. Ginsberg ~W. Sci., Singapore,
1993, Vol. III.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.MAR.V30.12
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