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We note that there are contradictory experiments that are interpreted to give a first order transition with a lattice constant discontinuity of 1%. However, those are closed cell thermodynamic systems and are not as conceptually simple as the experiments of
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We note that there are contradictory experiments that are interpreted to give a first order transition with a lattice constant discontinuity of 1%. However, those are closed cell thermodynamic systems and are not as conceptually simple as the experiments of Hamichi
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The values derived from the model potentials depend sensitively on the value of z that is used. The following results are the values at z that corresponds to the ground state (potential energy plus zero point energy) of V0 (z) for models of SUSCAS 0039-6028 10.1016/0039-6028(96)00821-7
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The values derived from the model potentials depend sensitively on the value of z that is used. The following results are the values at z that corresponds to the ground state (potential energy plus zero point energy) of V0 (z) for models of W. A. Steele, Surf. Sci. SUSCAS 0039-6028 10.1016/0039- 6028(96)00821-7 36, 317 (1973)
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The values are -3.8 K for the Steele model and -7.5 K for that of
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The values are -3.8 K for the Steele model and -7.5 K for that of Klein When the substrate anisotropy is included with γa =0.4 and γR =-0.54, the values change to -6.2 K (at z=3.72 Å) and -12.3 K (at z=3.39 Å), respectively.
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Klein1
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23
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PRBMDO 0163-1829 10.1103/PhysRevB.40.4797
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show a pattern of hexagonal Xe/ graphite domains at 5 K with walls tilted by 11° and spaced by 5 nm. If the walls are superlight, the structure has =0.54° and L=4.48 Å. Such a structure corresponds to one detected in electron diffraction by
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show a pattern of hexagonal Xe/ graphite domains at 5 K with walls tilted by 11° and spaced by 5 nm. If the walls are superlight, the structure has =0.54° and L=4.48 Å. Such a structure corresponds to one detected in electron diffraction by Hamichi (Ref.) at T/75 K.
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Hamichi1
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