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The specific heat of the three-dimensional Ising model below Tc

D S Gaunt and C Domb

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A representation for the specific heat below Tc of a three-dimensional Ising ferromagnet (or fluid) is constructed. On expansion, it yields the first twelve terms of the exact low-temperature series for the tetrahedral lattice, and behaves asymptotically as

equation

where αprime = fraction one-eighth, A- = 0centerdot20 and B- = 0centerdot13. However, such behaviour is only becoming evident at t identical with 1 - T/Tc similar, equals 10-4. Indeed, from t similar, equals 4 × 10-2 to 4 × 10-4, CH appears to be increasing roughly logarithmically.

The specific heat of the Ising model is compared directly with experimental results for four `classical' fluids and three Ising-like antiferromagnets. Difficulties in establishing experimental values for the critical exponent αprime are discussed.

A simple explanation is proposed of why the `rounding-off', observed in most magnetic transitions, is often more pronounced below Tc.


PACS

75.40.Cx Static properties (order parameter, static susceptibility, heat capacities, critical exponents, etc.)

75.10.Hk Classical spin models

75.30.Kz Magnetic phase boundaries (including magnetic transitions, metamagnetism, etc.)

Subjects

Condensed matter: electrical, magnetic and optical

Dates

Issue 4 (August 1968)

Received 15 February 1968



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