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gezelter |
1916 |
This directory contains a set of quadrupolar crystals that can be used |
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to test electrostatic energies for quadrupole-quadrupole interactions. |
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The quadrupolar analogues to the structural Madelung constants for |
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ionic crystals were first worked out by Nagai and Nakamura who |
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computed the energies of certain selected quadrupole arrays and |
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obtained a number of these constants.[1] Their work is based on |
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earlier work on dipolar crystals that was done by Luttinger & Tisza |
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[2]. We have generated only the lowest energy configurations for the |
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linear quadrupoles |
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Lattice Quadrupole Direction Energy constants Notes |
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------- -------------------- ---------------- ------ |
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SC 111 -8.30 Fig 6a |
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BCC 011 -21.7 Fig 7b |
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FCC 111 -80.5 Fig 8 |
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The electrostatic energy for one of these dipolar arrays is |
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E = C (3/4) N^2 Q^2 |
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where C is the energy constant above, N is the number of quadrupoles |
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per unit volume, and Q is the strength of the dipole. |
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gezelter |
1921 |
In the units used by OpenMD, with quadrupole moments of 1 |
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gezelter |
1916 |
Debye-angstrom, lengths in angstroms, and energies reported in |
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kcal / mol, the electrostatic energies are: |
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E = 14.39325 (3/4) C N^2 Q^2 |
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E here is an energy density, so it must be multiplied by the total |
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volume of the box. |
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--------------------------------------------------------------------- |
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[1] O. Nagai and T. Nakamura, "Quadrupole Interaction in Crystals," |
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Progress of Theoretical Physics 24 (2), 432-454 (1960) |
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gezelter |
1921 |
doi: 10.1143/PTP.24.432, also see Errata: Progress of |
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Theoretical Physics 30 (3), 412 (1963). doi: 10.1143/PTP.30.412a |
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gezelter |
1916 |
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[2] J. M. Luttinger and L. Tisza, "Theory of Dipole Interaction in |
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Crystals," Phys. Rev. 70, 954–964 (1946) doi: 10.1103/PhysRev.70.954 |