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Understanding the quadrupolar structures of UPd(3)

Authors
McEwen, KA[McEwen, K. A.]Walker, HC[Walker, H. C.]Le, MD[Le, M. D.]McMorrow, DF[McMorrow, D. F.]Colineau, E[Colineau, E.]Wastin, F[Wastin, F.]Wilkins, SB[Wilkins, S. B.]Park, JG[Park, J.-G.]Bewley, RI[Bewley, R. I.]Fort, D[Fort, D.]
Issue Date
Mar-2007
Publisher
ELSEVIER SCIENCE BV
Keywords
UPd(3); quadrupolar order; X-ray resonant scattering
Citation
JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, v.310, no.2, pp.718 - 722
Indexed
SCIE
SCOPUS
Journal Title
JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS
Volume
310
Number
2
Start Page
718
End Page
722
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/84847
DOI
10.1016/jmmm.2006.10.520
ISSN
0304-8853
Abstract
UPd(3) exhibits four phase transitions below T(0) = 7.8 K, attributed to a succession of antiferroquadrupolar (AFQ) orderings of the 5f(2) uranium ions localised on the quasi-cubic sites of the dhcp crystal structure. From earlier polarised neutron diffraction measurements in a magnetic field, we proposed that the order parameter of the phase below T(0) is Q(x2-y2) and a model for the order parameters of the four phases was subsequently developed. This model has now been tested experimentally with measurements of the azimuthal dependence of the intensities of the quadrupolar reflections in the different phases, by means of X-ray resonant scattering (XRS) studies at ESRF. The results indicate that the order parameter, in zero field, of the phase below T(0) is Q(zx). Our model provides an explanation for these apparently contradictory results. New measurements of the heat capacity of UPd3 at low temperatures have revealed the entropy changes at each of the four transitions. We find that the entropy changes (Delta S) at T(0) and T(+1) = 6.9 K are minimal, whereas Delta S is large at T(-1) = 6.7 K. From this information together with the new XRS results, we have extended our model to provide an explanation of the AFQ structures of UPd(3). (c) 2006 Elsevier B. V. All rights reserved.
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