1988
DOI: 10.1016/0304-8853(88)90179-5
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Magnetic phase transition in layered CsGd(MoO4)2

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Cited by 5 publications
(5 citation statements)
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“…It should be noticed, however, that the existence of CsGd-(MoO 4 ) 2 molybdate has long been known, and some thermal and magnetic properties were observed in several studies. [24][25][26][27] Contrary to that, the properties of CsEu(MoO 4 ) 2 are unknown in the literature.…”
Section: Introductionmentioning
confidence: 99%
“…It should be noticed, however, that the existence of CsGd-(MoO 4 ) 2 molybdate has long been known, and some thermal and magnetic properties were observed in several studies. [24][25][26][27] Contrary to that, the properties of CsEu(MoO 4 ) 2 are unknown in the literature.…”
Section: Introductionmentioning
confidence: 99%
“…The latter was subtracted using a procedure based on the modification of the specific heat of CsGd(MoO 4 q 2 . Previous studies in zero magnetic field [8] showed that at temperatures above 10 K, only lattice vibrations contribute to the CsGd(MoO 4 q 2 specific heat. Thus, using the ratio of Gd to Nd molar mass, being equal to 1.02, lattice contribution in CsNd(MoO 4 q 2 was estimated as C LAT (Nd)=1.02 ¢ C LAT (Gd).…”
Section: Resultsmentioning
confidence: 99%
“…Energy scheme (2) corresponds to the local symmetry D 2 with CEF parameters given in Table. 1 low-temperature data below 2 K [26] completed with the current measurements performed above 2 K. It is clear that the description of the data is not sufficient, pointing at the overestimation of the CEF influence. Thus, the effect of magnetic correlations and/or other low-symmetry terms in H CEF should be included.…”
Section: Crystal-field Symmetrymentioning
confidence: 99%
“…Besides their potential use in the optoelectronic devices at room-temperature applications, the compounds possess interesting magnetic properties at low temperatures [24,25]. Previous low-temperature studies [26,27,28,29,30,24] considered this material as a quasi-one dimensional dipolar magnet with a magnetic phase transition to the ordered state at T C = 0.45 K. The effective strength of dipolar interactions was estimated in the form of the effective intra-chain coupling parameter J/k B ≈ 0.6 K and interchain coupling J ′ < 0.03 J [27].…”
Section: Introductionmentioning
confidence: 99%
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