Two-level system the result of Problerrl4 is often seen in another form. (a) If the two energy
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Two-level system the result of Problerrl4 is often seen in another form.
(a) If the two energy levels are at Δ and – Δ, show that the energy and heat capacity are U = - Δ tanh (Δ/kBT); C = kB (Δ/kBT)2 sech2 (Δ/kBT).
(b) If the system has a random composition such that all values of Δ are equally likely up to some limit Δ0, show that the heat capacity is linearly proportional to the temperature, provided kBT << Δ0. This result was applied to the heat capacity of dilute magnetic alloys by W. Marshall, Phys. Rev. 118, 1519 (1960). It is also used in the theory of glasses.
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