Jw. Lynn et al., NATURE OF THE MAGNETIC ORDER IN SUPERCONDUCTING AND NONSUPERCONDUCTING HONI2-XCOXB2C, Physical review. B, Condensed matter, 53(2), 1996, pp. 802-808
Neutron-diffraction measurements have been carried out to investigate
the magnetic properties of superconducting (T-c similar to 8 K) HoNi2B
2C and nonsuperconducting (T-c<3 K) HoNi1.98Co0.015B2C. Both systems b
ecome magnetically long-range ordered below similar to 8 K, with three
types of magnetic order being present. The low-temperature structure
is a commensurate antiferromagnetic state that consists of Ho3+ moment
s aligned ferromagnetically in the a-b plane, with the sheets coupled
antiferromagnetically along the c axis. The magnetic state that initia
lly forms on cooling, however, is dominated by an incommensurate spira
l antiferromagnetic state along the c axis, with wave vector q(c) appr
oximate to-0.054 Angstrom(-1), in which the relative alignment of each
ferromagnetic sheet is rotated in the a-b plane by similar to 17 degr
ees from the low-temperature antiparallel configuration. The intensity
for this spiral state reaches a maximum near similar to 5 K; the spir
al state then collapses at lower temperature in favor of the commensur
ate antiferromagnetic state. A smaller amplitude a-axis modulation, wi
th q(a) approximate to 0.73 Angstrom(-1), is also observed above the s
piral antiferromagnetic transition, but over a narrower temperature ra
nge than the spiral state. The identical sequence of phase transitions
is observed for both the superconducting and nonsuperconducting sampl
es, demonstrating that the reentrant superconductivity and the coexist
ence of long-range antiferromagnetic order and superconductivity at lo
w temperatures are both controlled by the nature of the magnetic struc
tures present. In the temperature regime where the three magnetic stru
ctures are observed simultaneously, the sample dependence of the inten
sities strongly suggests that they occur in spatially separate regions
.