ELSEVIER Physica C 254 (1995) 124-130
PHYSICA
Magnetization studies on ErNi2B2C single crystals
R. Szymczak a,*, M. Baran a, L. Gtadczuk a, H. Szymczak a, Z. Drzazga b,
A. Winiarska b
a Institute of Physics, Polish Academy of Sciences, al. Lotnik6w 32/46, 02-668 Warsaw, Poland
b Institute of Physics, Silezian University, Katowice, Poland
Received 21 March 1995; revised manuscript received 28 June 1995
Abstract
The magnetization of single crystal ErNi2B2C has been measured in the temperature range from 2 K up to 200 K and in
magnetic fields up to 5 T. Performed measurements reveal a striking anisotropy both in paramagnetic and ordered states. It
has been suggested that the high susceptibility near the N6el temperature is responsible for anomalies observed in the
temperature dependence of the first field for flux penetration and for the irreversibility field. A cascade of metamagnetic
transitions has been observed for an external field applied perpendicular to the c-axis. These transitions are discussed in the
framework of the incommensurate mean-field model.
1. Introduction
The newly discovered [1-3] rare-earth quaternary
nickel boron carbide systems are model materials to
study the interplay between the competing effects of
superconductivity and magnetism. In this respect,
their properties are reminiscent of the rare-earth
rhodium borides and ternary molybdenum chalco-
genides (see Refs. [4] and [5], and references therein).
Particularly, a pronounced dip structure in the upper
critical-field temperature dependence Hc2(T) was
observed both in some of the new rare-earth nickel
boride carbides RENi2B2C [6-8] and in magnetic
superconductors RERh4B 4 and REM06S 8 [4,5]. Such
a dip was observed in RENi2B2C for RE = Ho and
* Corresponding author.
Er. Since the dip in the Hc2(T) curve indicates the
presence of strong pairbreaking near the N6el tem-
perature the magnetization studies seem to be impor-
tant to understand the role of magnetic structure and
magnetic interactions in this new family of supercon-
ductors. The availability of relatively large single
crystals [9] allows for studies of the anisotropy in
borocarbides. Such studies have been performed al-
ready for HoNi2B2C (see, for example, Refs. [7] and
[10]), therefore it was decided to carry out detailed
measurements of the magnetic and superconducting
properties of ErNi2B2C single crystals.
The magnetic structure of ErNi2B2C, as has been
already established [11,12], is associated with spins
of the Er atoms. They are ordered in a transversely
polarized planar sinusoidal structure, propagating
along the a- (or b-) axis in equal domains, with the
Er moments parallel to the b- (or a-) axis, respec-
tively.
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