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s = +1s = -1
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Phase diagrams of the 1/2-spin Ising model H=0 similar to phase diagrams of fluids
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EJERCICIO 9: except for T < T c
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sisi (1944)
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average field due to neighbouring spins external field effective field averaged magnetisation independent of dimensionality! Energy of i-th spin: Total energy: (factor 1/2 to avoid counting spin pairs twice) (quasi) ideal:
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rama metaestable región inestable DOMINIOS MAGNÉTICOS
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spinodal region nucleation region nucleation kinetics: nucleation barrier, critical domain size, growth by motion of grain boundaries spinodal decomposition: instability at q=0 (long- wavelength fluctuation)
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ordered
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(J>0)
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EJERCICIO 10 study the nature of the transition for |H| small
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EJERCICIO 11a
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EJERCICIO 11b
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Stirling's approx.
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Types of boundary conditions:
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diverges but only at T=0
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... 1
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A B A A B B A A B A B B A A B A A B A B B A B B A
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NaF/AlF 3 mixture
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structure of -brass, CuZn
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number of bonds probability of one neighbour being A probability of the other neighbour being B Now we make a mean-field approximation. the Bragg-Williams approximation:
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Entropic contribution. Favours mixing (disorder). Has minimum at x=1/2 (complete mixing) and maxima at x=0 and 1 (pure phases) Energetic contribution. Favours segregation (order). Has minima at x=0 and 1 (pure phases) and maximum at x=1/2 CONSTANTS HAVE BEEN DROPPED!
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