2005
DOI: 10.1103/physrevb.71.214418
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Magnetic susceptibility of aCuO2plane in theLa2CuO

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Cited by 17 publications
(47 citation statements)
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“…A few remarks are in order now concerning the usefulness of the NLSM approach to the model ͑2͒ with respect to other approaches. 8,9,11 First, the action ͑9͒ allows one to easily track down the source of the anisotropic magnetic response, as coming from the term B · ͑D + ϫ n͒. In fact, depending on the directions of D + and of the applied field, there will be ͑or not͒ additional terms proportional to G ␣ in Eq.…”
Section: Magnetic Susceptibilitymentioning
confidence: 99%
“…A few remarks are in order now concerning the usefulness of the NLSM approach to the model ͑2͒ with respect to other approaches. 8,9,11 First, the action ͑9͒ allows one to easily track down the source of the anisotropic magnetic response, as coming from the term B · ͑D + ϫ n͒. In fact, depending on the directions of D + and of the applied field, there will be ͑or not͒ additional terms proportional to G ␣ in Eq.…”
Section: Magnetic Susceptibilitymentioning
confidence: 99%
“…For example, when a small magnetic field is applied perpendicular to the layers the magnetic susceptibility shows a strong enhancement as the Néel temperature is approached, due to the formation of these ferromagnetic moments. 8,12,13 When the field strength is further enhanced one can observe a spin flop of the ferromagnetic moments with respect to the out-of-plane staggered order that they display at zero field. 8,10,11 Analogously the spin-flop transition of the staggered in-plane AF moments for a field along the easy axis is accompanied by unconventional effects related to the presence of the DM interaction.…”
Section: Introductionmentioning
confidence: 99%
“…8,10,11 Analogously the spin-flop transition of the staggered in-plane AF moments for a field along the easy axis is accompanied by unconventional effects related to the presence of the DM interaction. 9,10 Recently new theoretical approaches have been proposed [12][13][14] to integrate the semiclassical picture already presented in the prior work of Refs. 7-10.…”
Section: Introductionmentioning
confidence: 99%
“…2,8,25,41 Each plane carries a weak ferromagnetic moment ͑WFM͒ which orders antiparallel in adjacent layers for T Ͻ T N . When the external field H ʈ c exceeds the spin-flip field H SF needed to overcome the interlayer coupling J Ќ , the spin lattice of every other layer rotates by = 180°so that the WFMs of all planes become parallel to the field.…”
Section: Magnetizationmentioning
confidence: 99%