1984
DOI: 10.1016/0038-1098(84)90381-8
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On the problem of superdiamagnetism

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Cited by 117 publications
(79 citation statements)
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“…The extension to ferroelectrics was made around 1984 by Ginzburg et al [8] and was recently further developed using ab initio calculations by Naumov et al [9]. We note that toroidal domains can arise for two unrelated physical reasons: (1) finite size effects and boundary conditions (present work) and (2) magnetoelectric coupling in multiferroic materials [7,8,[10][11][12]. The present work does not involve magnetism.…”
mentioning
confidence: 69%
“…The extension to ferroelectrics was made around 1984 by Ginzburg et al [8] and was recently further developed using ab initio calculations by Naumov et al [9]. We note that toroidal domains can arise for two unrelated physical reasons: (1) finite size effects and boundary conditions (present work) and (2) magnetoelectric coupling in multiferroic materials [7,8,[10][11][12]. The present work does not involve magnetism.…”
mentioning
confidence: 69%
“…In the SC state, orbital antiferromagnetic (OAF) order [15,16,17,18,19] that can be associated with nonzero relative phase α of the SC order parameter develops as AF correlated orbital current circulations [20]. Such circulations may survive above T c in the form of either long-range [21] or short-range [22] OAF order.…”
Section: Spontaneous Orbital Currentsmentioning
confidence: 99%
“…It has been shown [7,8,9,10,11] that, without any other modifications, one can formally substitute T for v in figure 1. We can remark that this kind of configuration of currents can be created from a solenoidal configuration of currents.…”
Section: -Preliminariesmentioning
confidence: 99%
“…Thus, as it can be seen in the figure 1, only 31 magnetic groups are compatible with the existence of a relativistic crystalline symmetry (see the groups contained into the lowest circle). The invariant non-zero velocity vectors can be linked with toroidal moments from the point of view of magnetic symmetries as it has been already shown in previous papers [7,8]. In that one, we will explain how toroidal moments might be generated from broken relativistic crystalline symmetries and give a few assumptions in order to construct a superconductivity model.…”
mentioning
confidence: 99%