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Krakauer, H.1
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0001672358
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0001458846
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16
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85038909394
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is a package of molecular simulation routines written by W. Smith and T. R. Forester, Daresbury and Rutherford Appleton Laboratory, Daresbury, UK
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DL-POLY is a package of molecular simulation routines written by W. Smith and T. R. Forester, Daresbury and Rutherford Appleton Laboratory, Daresbury, UK.
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85038945201
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For convenience, we use the terms “phonons” or “normal modes” to refer to the eigenvectors of the force-constant matrix
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For convenience, we use the terms “phonons” or “normal modes” to refer to the eigenvectors of the force-constant matrix.
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85038964566
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When the simulations are performed decreasing the temperature, we find the same transition sequence with hysteresis in (formula presented)’s of less than 5 K
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When the simulations are performed decreasing the temperature, we find the same transition sequence with hysteresis in (formula presented)’s of less than 5 K.
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85038909756
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This approximation is known to be inappropriate for some systems. For example, the authors of Ref., found that nonlocal anharmonic couplings involving oxygen octahedron tilting variables are essential to reproduce the experimentally observed phase diagram of Zr-rich PZT
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This approximation is known to be inappropriate for some systems. For example, the authors of Ref. 9 found that nonlocal anharmonic couplings involving oxygen octahedron tilting variables are essential to reproduce the experimentally observed phase diagram of Zr-rich PZT.
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23
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85038909196
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Leung, (Ref. also considered an effective pressure varying linearly with temperature in order to incorporate thermal expansion in their effective-Hamiltonian study of Zr-rich PZT. Interestingly, the coefficient they used (formula presented) is very similar to the one that corresponds to the shell model of (formula presented) (formula presented)
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Leung et al. (Ref. 9) also considered an effective pressure varying linearly with temperature in order to incorporate thermal expansion in their effective-Hamiltonian study of Zr-rich PZT. Interestingly, the coefficient they used (formula presented) is very similar to the one that corresponds to the shell model of (formula presented) (formula presented)
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24
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85038914699
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N. W. Ashcroft and N. D. Mermin, (Saunders College Publishing, Philadelphia, 1976)
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N. W. Ashcroft and N. D. Mermin, Solid State Physics (Saunders College Publishing, Philadelphia, 1976).
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25
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85038908524
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One could think of computing (formula presented) for each of the phases of the system, which should then be treated separately in the simulation
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One could think of computing (formula presented) for each of the phases of the system, which should then be treated separately in the simulation.
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