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- W1982579088 abstract "Quantum melting of a ferroelectric moment in the frustrated hydrogen-bonded system with the ``ice rule'' is studied theoretically by using quantum Monte Carlo simulation. The large number of nearly degenerate configurations are described as the gauge degrees of freedom; i.e., the model is mapped to a lattice gauge theory, which shows the confinement-deconfinment transition (CDT). The dipole-dipole interaction ${J}_{2}$, on the other hand, explicitly breaks the gauge symmetry leading to the ferroelectric transition at finite temperature $T$. It is found that the crossover from the FT to CDT manifests itself in the reduced correlation length of the polarization ${ensuremath{xi}}_{mathrm{FT}}ensuremath{sim}mathrm{ensuremath{Delta}}(Kensuremath{-}{K}_{c}{)}^{ensuremath{-}ensuremath{nu}}$, with $mathrm{ensuremath{Delta}}ensuremath{propto}sqrt{{J}_{2}}$ while ${K}_{c}$ and $ensuremath{nu}$ remains finite in the limit ${J}_{2}ensuremath{rightarrow}0$. In contrast, the Curie-Weiss-like law for the susceptibility $ensuremath{chi}$ and the spontaneous polarization behaves smoothly and the length scale ${ensuremath{xi}}_{mathrm{CDT}}$, related to the molecular symmetry and volume for CDT, does not reduce in this limit." @default.
- W1982579088 created "2016-06-24" @default.
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- W1982579088 date "2014-06-17" @default.
- W1982579088 modified "2023-10-16" @default.
- W1982579088 title "Gauge Field and the Confinement-Deconfinement Transition in Hydrogen-Bonded Ferroelectrics" @default.
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- W1982579088 doi "https://doi.org/10.1103/physrevlett.112.247602" @default.
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