4.8 Article

Proton strings and rings in atypical nucleation of ferroelectricity in ice

Publisher

NATL ACAD SCIENCES
DOI: 10.1073/pnas.2018837118

Keywords

ice; ferroelectricity; nucleation; proton strings and rings; replica exchange Monte Carlo

Funding

  1. Consejo Nacional de Investigaciones Cient'ificas y Tecnicas, Argentina
  2. European Research Council [8344023]
  3. Italian Ministry of University and Research through PRIN UTFROM Research Grant [20178PZCB5]

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Research has shown that light doping with KOH at low temperature leads to a transition to ferroelectric ice, but the microscopic mechanism behind this transition still needs further clarification. A lattice model based on dipolar interactions was introduced to explain this phenomenon, highlighting the impact of proton ring configurations on the stability of ice.
Ordinary ice has a proton-disordered phase which is kinetically metastable, unable to reach, spontaneously, the ferroelectric (FE) ground state at low temperature where a residual Pauling entropy persists. Upon light doping with KOH at low temperature, the transition to FE ice takes place, but its microscopic mechanism still needs clarification. We introduce a lattice model based on dipolar interactions plus a competing, frustrating term that enforces the ice rule (IR). In the absence of IR-breaking defects, standard Monte Carlo (MC) simulation leaves this ice model stuck in a state of disordered proton ring configurations with the correct Pauling entropy. A replica exchange accelerated MC sampling strategy succeeds, without open path moves, interfaces, or off-lattice configurations, in equilibrating this defect-free ice, reaching its low-temperature FE order through a well-defined first-order phase transition. When proton vacancies mimicking the KOH impurities are planted into the IR-conserving lattice, they enable standard MC simulation to work, revealing the kinetics of evolution of ice from proton disorder to partial FE order below the transition temperature. Replacing ordinary nucleation, each impurity opens up a proton ring generating a linear string, an actual FE hydrogen bond wire that expands with time. Reminiscent of those described for spin ice, these impurity-induced strings are proposed to exist in doped water ice too, where IRs are even stronger. The emerging mechanism yields a dependence of the long-time FE order fraction upon dopant concentration, and upon quenching temperature, that compares favorably with that known in real-life KOH doped ice.

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