Issue |
Europhys. Lett.
Volume 53, Number 3, February 2001
|
|
---|---|---|
Page(s) | 354 - 359 | |
Section | Condensed matter: electronic structure, electrical, magnetic, and optical properties | |
DOI | https://doi.org/10.1209/epl/i2001-00161-8 | |
Published online | 01 December 2003 |
A new heavy-fermion superconductor
: A relative of the
cuprates?
1
Condensed Matter and Thermal Physics, Los Alamos National
Laboratory Los Alamos, NM 87545 USA
2
National High Magnetic Field Laboratory, Florida State University
Tallahassee, FL 32306 USA
Corresponding author: jdt@mst.lanl.gov
Received:
18
July
2000
Accepted:
22
November
2000
is a member of a new family of heavy-fermion compounds
and has a Sommerfeld specific-heat coefficient of
. It exhibits
a bulk, thermodynamic transition to a superconducting state at
, below which the specific heat decreases as T2 to a small residual
T-linear value. Surprisingly, the electrical resistivity drops below instrumental
resolution at a much higher temperature
. These behaviors are highly
reproducible and field-dependent studies indicate that T0 and
arise
from the same underlying electronic structure. The layered crystal structure of
suggests a possible analogy to the cuprates in which spin/charge
pair correlations develop well above
.
PACS: 71.27.+a – Strongly correlated electron systems; heavy fermions / 74.70.Tx – Heavy-fermion superconductors
© EDP Sciences, 2001
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