1995
DOI: 10.1016/0304-8853(94)01177-x
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Magnetic ordering in CsCuCl3

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1995
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Cited by 19 publications
(21 citation statements)
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“…Nevertheless, the critical exponent b ¼ 0.25(1) has been obtained in Ref. [19] in agreement with the XY chiral scenario [5], although, according to Ref. [18], b ¼ 0.358(15) is close to a non-chiral XY model.…”
Section: Interplay Between the Dzyaloshinskii Vector The Spin Chiralsupporting
confidence: 58%
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“…Nevertheless, the critical exponent b ¼ 0.25(1) has been obtained in Ref. [19] in agreement with the XY chiral scenario [5], although, according to Ref. [18], b ¼ 0.358(15) is close to a non-chiral XY model.…”
Section: Interplay Between the Dzyaloshinskii Vector The Spin Chiralsupporting
confidence: 58%
“…[18,19]. Following the arguments [18], only one magnetic satellite of the ( be observed according to Eq.…”
Section: Interplay Between the Dzyaloshinskii Vector The Spin Chiralmentioning
confidence: 94%
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“…Both have their own associated fascinating ground state physics, but still consist of stronger Heisenberg ferromagnetic correlations in 1D with weaker antiferromagnetic exchange between the ferromagnetic chains. [33,34] An interesting result in 1D magnetism can be found in the compounds Sr 3 CuIrO 6 and Sr 3 CuPtO 6 , which are 1D Heisenberg ferromagnetic and antiferromagnetic, respectively. Mixing of the two materials results in a random ferro/antiferromagnetic paramagnetic state, described as a quantum spin chain paramagnet.…”
Section: (A) Frustrated Magnetism and Magnetic Systemsmentioning
confidence: 99%
“…Introducing a "squash" mapping, we show that the magnetic properties of coupled spin chains can be phenomenologically described by a single-layer TLAF model with effective spinS. The crucial experimental step is a series of precise magnetic measurements conducted under high pressure up to P = 1.21 GPa on a CsCuCl 3 single crystal [35][36][37][38][39][40][41] , which allows us to determine the exchange couplings to great accuracy and, consequently, extract the parameters of the effective model. We thus demonstrate that the value of effective spinS can be actually controlled by external pressure through the change in the material parameters.…”
mentioning
confidence: 99%