3. Consider a 2 × 2 square lattice of spins interacting via the Ising Hamiltonian in the absence of a magnetic field: H = - ΣSi Sj, (ij) we have set J = 1. (a) Write down all the possible configurations and calculate the energy for each one of them. (b) Calculate the partition function Z, as a function of temperature, by summing over all configurations. (c) Repeat question (3a) and (3b), using periodic boundary condi- tions.

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3. Consider a 2 × 2 square lattice of spins interacting via the Ising
Hamiltonian in the absence of a magnetic field:
H =
-
ΣSi Sj,
(ij)
we have set J = 1.
(a) Write down all the possible configurations and calculate the energy
for each one of them.
(b) Calculate the partition function Z, as a function of temperature,
by summing over all configurations.
(c) Repeat question (3a) and (3b), using periodic boundary condi-
tions.
Transcribed Image Text:3. Consider a 2 × 2 square lattice of spins interacting via the Ising Hamiltonian in the absence of a magnetic field: H = - ΣSi Sj, (ij) we have set J = 1. (a) Write down all the possible configurations and calculate the energy for each one of them. (b) Calculate the partition function Z, as a function of temperature, by summing over all configurations. (c) Repeat question (3a) and (3b), using periodic boundary condi- tions.
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