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M. A. de Vries,1,* D. Wulferding,2 P. Lemmens,2 J. S. Lord,3 A. Harrison,1,4 P. Bonville,5 F. Bert,6 and P. Mendels6 1CSEC and School of Chemistry, The University of Edinburgh, Edinburgh EH9 3JZ, United Kingdom 2Institute for Condensed Matter Physics, TU Braunschweig, Mendelssohnsstrasse 3, D-38106 Braunschweig, Germany 3ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot, Oxon OX11 OQX, United Kingdom 4Institut Laue-Langevin, 6 rue Jules Horowitz, F-38000 Grenoble, France 5Service de Physique de l’État Condensé, DSM, CEA Saclay, F-91191 Gif-sur-Yvette Cedex, France 6Laboratoire de Physique des Solides, Universite Paris X, Orsay, France (Received 9 November 2011; revised manuscript received 8 January 2012; published 20 January 2012)

physical review b

Extension of the zinc paratacamite phase diagram: Probing the effect of spin vacancies in an<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mn>2</mml:mn></mml:mfrac></mml:mrow></mml:math>kagome antiferromagnet

Extension of the zinc paratacamite phase diagram: Probing the effect of spin vacancies in anS=12kagome antiferromagnet