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Correlation between the structural and antiferromagnetic phase transitions in ZnCr 2 Se 4
Author(s) -
Hidaka M.,
Tokiwa N.,
Fujii M.,
Watanabe S.,
Akimitsu J.
Publication year - 2003
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.200301502
Subject(s) - antiferromagnetism , condensed matter physics , orthorhombic crystal system , neutron diffraction , phase transition , ferromagnetism , magnetic structure , materials science , crystallography , crystal structure , magnetization , chemistry , physics , magnetic field , quantum mechanics
Structural properties of normal‐type spinel ZnCr 2 Se 4 have been studied as a function of temperature by means of neutron diffraction. It is found that the structural phase transition ( T C ) from a cubic to orthorhombic symmetry simultaneously occurs at the antiferromagnetic phase transition temperature ( T N ∼ 21 K), where the cubic and orthorhombic symmetry is 7 O h ‐Fd3m and 24 D 2h ‐Fddd, respectively. The structural phase transition is mainly characterized by the cooperative displacements of Se 2– ions, which are induced by a magnetostriction resulting from the magnetic interaction of Cr 3+ ions in CrSe 4 chains along [110]. The antiferromagnetic magnetic structure below T N is made by a spiral magnetic coupling between the ferromagnetic CrSe 4 chains around crystallographic screw axes, which are parallel to an orthorhombic C axis. The spiral long‐range order of the spins of Cr 3+ is incommensurate and its periodicity of q along a reciprocal lattice axis C * shows temperature dependence from about 0.47 (2.5 K) to 0.43 (18 K). The spiral periodicity of the spin order along the C axis shows a first order transition at about 21 K.
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