Europhys. Lett., 61 (4) , pp. 534-540 (2003)
Quantum phase transition in
to
collinear non-spin-flop state in magnetic field:
A neutron diffraction study
V. P. Plakhty1, S. V. Maleyev1, S. V. Gavrilov1, F. Bourdarot2, 3, S. Pouget2, 3 and S. N. Barilo4
1 Petersburg Nuclear Physics Institute RAS - Gatchina, 188300 St. Petersburg, Russia
2 CEA-Grenoble, DRFMC/SPSMS/MDN - 38042 Grenoble Cedex 9, France
3 Institut Laue-Langevin - BP 156, 38042 Grenoble Cedex 9, France
4 Institute for Solid State and Semiconductor Physics BYAS - 220072 Minsk, Belarus
(Received 17 July 2002; accepted in final form 4 December 2002)
Abstract
In the external field applied to the tetragonal antiferromagnet
, a transition is discovered from the phase with
orthogonal antiferromagnetic spin subsystems along
[1,0,0] and
[0,1,0] to the phase with collinear spins, which are
inclined about
to the field. This phase is shown to be
due to the interplane pseudodipolar interaction, and transforms
into the spin-flop phase
asymptotically at
very high field. The discovered phase transition is of first
order, if the field is along
[1,0,0], or
[0,1,0], and becomes
of second order if the field is slightly inclined to these axes.
It holds at
T = 0 and is a quantum one, with the transition
field being the critical point and the angle between two
subsystems below the critical point being the order parameter.
75.25.+z - Spin arrangements in magnetically ordered materials (including neutron and spin-polarized electron studies, synchrotron-source X-ray scattering, etc.).
75.30.Kz - Magnetic phase boundaries (including magnetic transitions, metamagnetism, etc.).
75.50.Ee - Antiferromagnetics.
© EDP Sciences 2003


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