2003
DOI: 10.1103/physrevb.67.064401
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Magnetism of pure iron jarosites

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Cited by 96 publications
(190 citation statements)
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References 48 publications
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“…The room-temperature structure was solved in space group R3m using direct methods. The space group choice R3m (R int = 0.034) is in agreement with previous single-crystal studies of Na jarosite and H 3 O jarosite (Grohol et al 2003;Nestola et al 2013;Majzlan et al 2004;Plášil et al 2014;Spratt et al 2014).…”
Section: Crystal Structure Refinementsupporting
confidence: 77%
“…The room-temperature structure was solved in space group R3m using direct methods. The space group choice R3m (R int = 0.034) is in agreement with previous single-crystal studies of Na jarosite and H 3 O jarosite (Grohol et al 2003;Nestola et al 2013;Majzlan et al 2004;Plášil et al 2014;Spratt et al 2014).…”
Section: Crystal Structure Refinementsupporting
confidence: 77%
“…The energy integrated neutron scattering cross-section is proportional to the instantaneous spin correlator (16) and provides an experimental tool for its measurement. Previous numerical works on the kagome antiferromagnet have considered only the powder averaged structure factor.…”
Section: 7mentioning
confidence: 99%
“…The D 4h symmetry of the ligand field was lowered to C 2 to model the actual positions of the oxygen anions around the cation, as obtained from crystallographical data. 11,17 However, this had no effect on the agreement of the calculated spectra with experiment nor on the values as listed in Table I, and hence we consider an estimate for E xy from our data presently not attainable. It should in this respect be noted that the value for D z was found to change with the splitting of the main peak at 709 meV introduced by the trigonal distortion of the ligand field.…”
Section: Ligand-field Multiplet Calculationsmentioning
confidence: 66%
“…Potassium iron jarosite is representative for most of the iron analogs. In this system a transition to a noncollinear long-range-ordered state is observed at 64 K despite that the magnitude of the Curie-Weiss temperature ⌰ CW is as high as −800 K. 11,17 The ground state has shown to be a so-called q = 0 state of positive chirality, in which the spins lie within the kagome plane and all point either in or out of each shared kagome triangle. 9,12,13,18,19 The large figure ⌰ CW / T N = 12.5 is an indication of relatively strong geometric frustration, 20 but clearly the observed longrange-ordered ground state points to additional terms in the Hamiltonian of this kagome antiferromagnet beyond nearneighbor exchange.…”
Section: Introductionmentioning
confidence: 92%
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