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Symmetry-broken crystal structure of elemental boron at low temperature With Marek Mihalkovic (Slovakian Academy of Sciences) Outline: Cohesive energy puzzle (E < E ?) Optimization of partial occupancy in Symmetry-restoring phase transition
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Bond lengths: Occupancy: 100% 75% 9% 7% 27% 4%
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The structure of elemental Boron -B.hR12McCarty (1958, powder, red) -B.tP50Hoard (1958, 56 reflections, R=0.114) -B.hR105Geist (1970, 350 reflections, R=0.074) -B.hR111Callmer (1977, 920 reflections, partial occ. R=0.053) -B.hR141Slack (1988, 1775 reflections, partial occ. R=0.041) The energies of elemental Boron (relaxed DFT-GGA) -B.hR12 E = 0.00 (meV/atom) -B.tP50 E = +91.91 -B.hR105 E = +25.87 105 atoms/105 sites -B.hR111 E = +0.15 106 atoms/111 sites -B.hR141 E = 0.86 107 atoms/141 sites -B.aP214 E = 1.75 214 atoms/214 sites 3 rd law of thermodynamics!
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Stability of -Boron Possibility of Finite T phase transition (Runow, 1972; Werheit and Franz, 1986) Vibrational entropy can drive transition (Masago, Shirai and Katayama-Yoshida, 2006) Quantum zero point energy can stabilize (van Setten, Uijttewaal, de Wijs and de Groot, 2007) Symmetry-broken ground state , symmetric phase restored by configurational entropy (Widom and Mihalkovic, 2008)
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Occupancy: 100%75% 9%7% 27% 4% 100% cell center, partial occupancy All sites Optimal sites Clock model
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Structure and fluctuations Optimized structure Molecular dynamics T=2000K, duration 12ps
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2x1x1 Supercell Clock Model: “Time” shows occupancies Optimal times 02:20 and 10:00 Other times are low-lying excited states
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Symmetry-restoring phase transition of clock model { } = {all distinct clock configurations in 2x1x1 supercell} = degeneracy of configuration C TS U
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Conclusions E > E conflicts with observation of as stable Optimizing partial occupancy brings E < E Symmetry broken at low temperature (3 rd law) Symmetry restored through phase transition stabilized by entropy of partial occupation
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