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Spin-glass behavior of A Fe sub 4 Al sub 8 ( A =Th,U,Np) intermetallics

Journal Article · · Physical Review, B: Condensed Matter; (USA)
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  1. Nuclear Engineering Department, Ben-Gurion-University of the Negev, 84105 Beer Sheva (Israel) Nuclear Research Center, 84190 Beer-Sheva (Israel) Physik Department E15, Technische Universitaet Muenchen, D-8046 Garchingbei Muenchen (West Germany)
  2. Nuclear Engineering Department, Ben-Gurion-University of the Negev, 84105 Beer Sheva (Israel) Nuclear Research Center, 84190 Beer-Sheva (Israel)
  3. Physik Department E15, Technische Universitaet Muenchen, D-8046 Garching bei Muenchen (West Germany)
  4. Institut fuer Metallphysik, Technische Universitaet Braunschweig, D-3000 Braunschweig (West Germany) Physik Department E15, Technische Universitaet Muenchen, D-8046 Garching bei Muenchen (West Germany)
  5. Mineralogisches Institut der Universitaet Bonn, D-5300 Bonn (West Germany) Kernforschonganlage, D-5170 Juelich (West Germany)

Combined ac- and dc-susceptibility, neutron-diffraction, and Moessbauer studies of UFe{sub 4}Al{sub 8}, NpFe{sub 4}Al{sub 8}, and ThFe{sub 4}Al{sub 8} argue for the establishment of a spin-glass (SG) state below {ital T}{sub SG}({ital B}{r arrow}0){approx}130, 120, and 110 K, respectively. The SG temperature {ital T}{sub SG}({ital B}) decreases with application of external magnetic field {ital B}. The ac susceptibility ({chi}{sub ac}) shows a sharp cusp at {ital T}{sub SG}({ital B}{approx}0). The isothermal and thermoremanent magnetization differ markedly and show temperature-dependent irreversibilities below {ital T}{sub SG}({ital B}). The Moessbauer spectra reveal onset of hyperfine splitting, indicating frozen spins below {ital T}{sub SG}(0). The neutron-diffraction studies of UFe{sub 4}Al{sub 8} and NpFe{sub 4}Al{sub 8} show that after switching off the external magnetic field greater than 3 T the U and Np momenta (2{ital a} site) are frozen parallel to the direction of the external field. We label the freezing temperature under high external fields {ital T}{sub OG}, and show that it serves as the upper limit of {ital T}{sub SG}({ital B}) with {ital T}{sub SG}({ital B}{r arrow}0){r arrow}{ital T}{sub OG}. For concentrated SG systems, {ital T}{sub SG}(0) is a reproducible value, independent of the observation time window, which indicates a true thermodynamic phase transition; the cusp in {chi}{sub ac}, however, is not necessarily a confirmation for the establishment of a SG state.

OSTI ID:
6003774
Journal Information:
Physical Review, B: Condensed Matter; (USA), Journal Name: Physical Review, B: Condensed Matter; (USA) Vol. 42:13; ISSN PRBMD; ISSN 0163-1829
Country of Publication:
United States
Language:
English