S=1/2 Ising behavior in the two-dimensional molecular magnet Fe(NCS)2(pyrazine)2 -: art. no. 224405

被引:27
作者
Bordallo, HN
Chapon, L
Manson, JL
Hernández-Velasco, J
Ravot, D
Reiff, WM
Argyriou, DN
机构
[1] Hahn Meitner Inst Berlin GmbH, D-14109 Berlin, Germany
[2] Argonne Natl Lab, Intense Pulsed Neutron Source, Argonne, IL 60439 USA
[3] Rutherford Appleton Lab, ISIS Dept, Didcot OX11 0QX, Oxon, England
[4] Oak Ridge Natl Lab, Ctr Neutron Scattering, Oak Ridge, TN 37831 USA
[5] Eastern Washington Univ, Dept Chem & Biochem, Cheney, WA 99004 USA
[6] Univ Montpellier 2, Lab Physicochim Mat Condensee, CNRS, UMR 5617, F-34095 Montpellier 5, France
[7] Northeastern Univ, Dept Chem, Boston, MA 02115 USA
关键词
D O I
10.1103/PhysRevB.69.224405
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The magnetic ordering and critical behavior of antiferromagnetic Fe(NCS)(2)(pyrazine)(2) has been studied by neutron powder diffraction (NPD), inelastic neutron scattering (INS), Mossbauer spectroscopy, and magnetic measurements. The system can be regarded as a two-dimensional (2D) antiferromagnet even in the ordered phase, given that long-range magnetic ordering between the layers simply follows a necessary consequence of the establishment of long-range ordering within the planes. The INS data, which were taken on a cold neutron time-of-flight spectrometer, reveals that when the temperature is lowered towards T-N, the correlation length within the 2D layers increases and ultimately crosses over from two- to three-dimensional (3D) behavior. Indeed, 3D long-range antiferromagnetic order, associated with a propagation vector [1,0,1/4+epsilon], is observed in the NPD data below 6.8 K. Furthermore, in agreement with the behavior of both chi(T) and C-m(T) data, the order parameter follows the exact Osanger solution for a 2D S=1/2, Ising system.
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页码:224405 / 1
页数:9
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