Julien Autebert, Aditya Kashyap, et al.
Langmuir
We present and solve exactly a lattice model for magnetic or for structural phase transitions. The model proposed here can be seen as an extension of the spherical model. We obtain the following results: (i) The free energy of the system is calculated rigorously in a general case for lattices of any dimensionality d or structure. (ii) The critical properties are worked out explicitly for a special case of the interaction on a cubic d-dimensional lattice (d may be a fractional number). If d>2, second-order phase transitions may occur. The critical exponents are those of the sperical model. (iii) For a special choice of the interaction and if d3, the existence of a line of tricritical points can be demonstrated. The tricritical exponents are computed explicitly; they are identical to the exponents of the "Gaussian" model. (iv) Finally, first-order phase transitions are shown to exist in one and two dimensions. © 1977 The American Physical Society.
Julien Autebert, Aditya Kashyap, et al.
Langmuir
A.B. McLean, R.H. Williams
Journal of Physics C: Solid State Physics
Oliver Schilter, Alain Vaucher, et al.
Digital Discovery
M.A. Lutz, R.M. Feenstra, et al.
Surface Science