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Thermal corrections to the gap proportional to ω03 Tln [T/ (S ω0)] / D2 from the Hartree-Fock diagram and from the loop diagram discussed in Sec. 3 cancel each other. As a result, the thermal correction to the square of the gap for S∼1 is much smaller, ω03 T3/2 / D5/2 (see discussion in Sec. 3). To find it, one should take into account O (k2) corrections in the expansion of the dipolar tensor Qk ρβ, which depend on the lattice type.
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Thermal corrections to the gap proportional to ω03 Tln [T/ (S ω0)] / D2 from the Hartree-Fock diagram and from the loop diagram discussed in Sec. 3 cancel each other. As a result, the thermal correction to the square of the gap for S∼1 is much smaller, ω03 T3/2 / D5/2 (see discussion in Sec. 3). To find it, one should take into account O (k2) corrections in the expansion of the dipolar tensor Qk ρβ, which depend on the lattice type.
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Although TC given by Eq. 51 can differ several times from the real value of the Curie temperature (Ref.), this precision is sufficient for our estimations.
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Although TC given by Eq. 51 can differ several times from the real value of the Curie temperature (Ref.), this precision is sufficient for our estimations.
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Notice that even at large enough dipolar characteristic energy ω0 (remains small as compared to the exchange value), say, at ω0 ≈0.1J, we have Sln { 4πS (D/ [S ω0]) 3/2 } only for pretty large spins S8.
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