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Phys. Rev. B 74, 085112 (2006) [12 pages]

Unidirectional diagonal order and three-dimensional stacking of charge stripes in orthorhombic Pr1.67Sr0.33NiO4 and Nd1.67Sr0.33NiO4

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M. Hücker1, M. v. Zimmermann2, R. Klingeler3, S. Kiele3, J. Geck3, S. N. Bakehe4, J. Z. Zhang1,5, J. P. Hill1, A. Revcolevschi6, D. J. Buttrey7, B. Büchner3, and J. M. Tranquada1
1Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA
2Hamburger Synchrotronstrahlungslabor HASYLAB at Deutsches Elektronen-Synchrotron, 22603 Hamburg, Germany
3Leibniz-Institute for Solid State and Materials Research IFW Dresden, 01171 Dresden, Germany
4II. Physikalisches Institut, Universität zu Köln, 50937 Köln, Germany
5Cornell University, Ithaca, New York 14850, USA
6Laboratoire de Physico-Chimie de l’Etat Solide, Université Paris-Sud, 91405 Orsay Cedex, France
7Department of Chemical Engineering, University of Delaware, Newark, Delaware 19716, USA

Received 25 April 2006; published 15 August 2006

The interplay between crystal symmetry and charge stripe order in Pr1.67Sr0.33NiO4 and Nd1.67Sr0.33NiO4 has been studied by means of single crystal x-ray diffraction. In contrast to tetragonal La1.67Sr0.33NiO4, these crystals are orthorhombic. The corresponding distortion of the NiO2 planes is found to dictate the direction of the charge stripes, similar to the case of diagonal spin stripes in the insulating phase of La2−xSrxCuO4. In particular, diagonal stripes seem to always run along the short a axis, which is the direction of the octahedral tilt axis. In contrast, no influence of the crystal symmetry on the charge stripe ordering temperature itself was observed, with TCO∼240 K for La, Pr, and Nd. The coupling between lattice and stripe degrees of freedom allows one to produce macroscopic samples with unidirectional stripe order. In samples with stoichiometric oxygen content and a hole concentration of exactly 1∕3, charge stripes exhibit a staggered stacking order with a period of three NiO2 layers, previously only observed with electron microscopy in domains of mesoscopic dimensions. Remarkably, this stacking order starts to melt about 40 K below TCO. The melting process can be described by mixing the ground state, which has a three-layer stacking period, with an increasing volume fraction with a two-layer stacking period.

© 2006 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.74.085112
DOI:
10.1103/PhysRevB.74.085112
PACS:
71.45.Lr, 61.10.Nz, 61.72.Nn, 74.72.Dn