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Phys. Rev. B 63, 134433 (2001) [10 pages]

Magnetization measurements of antiferromagnetic domains in Sr2Cu3O4Cl2

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Beth Parks
Department of Physics and Astronomy, Colgate University, Hamilton, New York 13346

M. A. Kastner
Department of Physics and Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

Y. J. Kim
Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

A. B. Harris
Department of Physics, University of Pennsylvania, Philadelphia, Pennsylvania 19104

F. C. Chou
Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

O. Entin-Wohlman
School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Tel Aviv University, Tel Aviv 69978, Israel

Amnon Aharony
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Tel Aviv University, Tel Aviv 69978, Israel

Received 1 November 2000; published 15 March 2001

The Cu3O4 layer in Sr2Cu3O4Cl2 is a variant of the square CuO2 lattice of the high-temperature superconductors, in which the center of every second plaquette contains an extra Cu2+ ion. Whereas the ordering of the spins in the ground-state and the spin-wave excitations of this frustrated spin system are both well understood, we find peculiar behavior resulting from antiferromagnetic domain walls. Pseudodipolar coupling between the two sets of Cu2+ ions results in a ferromagnetic moment, the direction of which reflects the direction of the antiferromagnetic staggered moment, allowing us to probe the antiferromagnetic domain structure. After an excursion to the high fields (>1T), as the field is lowered, we observe the growth of domains with ferromagnetic moment perpendicular to the field. This gives rise to a finite domain wall susceptibility at small fields, which diverges near 100 K, indicating a phase transition. We also find that the shape of the sample influences the domain-wall behavior.

© 2001 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.63.134433
DOI:
10.1103/PhysRevB.63.134433
PACS:
05.70.Fh, 75.25.+z, 75.30.Cr, 75.60.-d