The anomalous skin effect in single crystal relaxor ferroelectric PZN-xPT and PMN-xPT
Authors:
G. Xu a;
P. M. Gehring b;
C. Stock c;
K. Conlon d
| Affiliations: | a Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973-5000 |
| b NIST Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, Maryland 20899-8562 | |
| c Department of Physics and Astronomy, Johns Hopkins University, Baltimore, MD, 21218 | |
| d Atomic Energy Canada Limited, Chalk River Laboratories, Chalk River Ontario, K0J 1J0 Canada |
DOI:
10.1080/02652030600558682
Publication Frequency:
12 issues per year
Subjects:
Condensed Matter Physics;
Crystallography;
Geophysics;
Materials Science;
Metals & Alloys;
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Abstract
X-ray and neutron scattering studies of the lead-based family of perovskite relaxors Pb(Zn1/3Nb2/3)O3-xPbTiO3 (PZN-xPT) and Pb(Mg1/3Nb2/3)O3-xPbTiO3 (PMN-xPT) have documented a highly unusual situation in which the near-surface region of a single crystal can exhibit a structure that is different from that of the bulk when cooled to low temperatures. The near-surface region, or “skin” can also display critical behavior that is absent in the crystal interior, as well as a significantly different lattice spacing. By varying the incident photon energy, and thus the effective penetration depth, X-ray measurements indicate a skin thickness of order 10-50 µm for PZN-xPT samples with 0 ≤ x ≤ 8%. Neutron residual stress measurements on a large PMN single crystal reveal a uniform lattice spacing within the bulk, but an increased strain near the surface. The presence of this skin effect has led to incorrect phase diagrams for both the PZN-xPT and PMN-xPT systems and erroneous characterizations of the nature of the relaxor state.
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| Keywords: PACS numbers: 77.80.-e; 77.84.Dy; 61.12.Ex; 61.10.Nz |
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