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Nature of the magnetic order in superconducting and nonsuperconducting HoNi{sub 2{minus}{ital x}}Co{sub {ital x}}B{sub 2}C

Journal Article · · Physical Review, B: Condensed Matter
;  [1];  [1]; ; ;  [2]
  1. Reactor Radiation Division, National Institute of Standards and Technology, Gaithersburg, Maryland 20899 (United States)
  2. ATT Bell Laboratories, Murray Hill, New Jersey 07974 (United States)

Neutron-diffraction measurements have been carried out to investigate the magnetic properties of superconducting ({Tc}{approximately}8 K) HoNi{sub 2}B{sub 2}C and nonsuperconducting ({Tc}{lt}3 K) HoNi{sub 1.985}Co{sub 0.015}B{sub 2}C. Both systems become magnetically long-range ordered below {approximately}8 K, with three types of magnetic order being present. The low-temperature structure is a commensurate antiferromagnetic state that consists of Ho{sup 3+} moments aligned ferromagnetically in the {ital a}-{ital b} plane, with the sheets coupled antiferromagnetically along the {ital c} axis. The magnetic state that initially forms on cooling, however, is dominated by an incommensurate spiral antiferromagnetic state along the {ital c} axis, with wave vector {ital q}{sub {ital c}}{approx_equal}0.054 {ital A}{sup {minus}1}, in which the relative alignment of each ferromagnetic sheet is rotated in the {ital a}-{ital b} plane by {approximately}17{degree} from the low-temperature antiparallel configuration. The intensity for this spiral state reaches a maximum near {approximately}5 K; the spiral state then collapses at lower temperature in favor of the commensurate antiferromagnetic state. A smaller amplitude {ital a}-axis modulation, with {ital q}{sub {ital a}}{approx_equal}0.73 {ital A}{sup {minus}1}, is also observed above the spiral antiferromagnetic transition, but over a narrower temperature range than the spiral state. The identical sequence of phase transitions is observed for both the superconducting and nonsuperconducting samples, demonstrating that the reentrant superconductivity and the coexistence of long-range antiferromagnetic order and superconductivity at low temperatures are both controlled by the nature of the magnetic structures present. In the temperature regime where the three magnetic structures are observed simultaneously, they occur in spatially separate regions. {copyright} {ital 1996 The American Physical Society.}

OSTI ID:
459845
Journal Information:
Physical Review, B: Condensed Matter, Journal Name: Physical Review, B: Condensed Matter Journal Issue: 2 Vol. 53; ISSN PRBMDO; ISSN 0163-1829
Country of Publication:
United States
Language:
English

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