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S = +1s = -1. Phase diagrams of the 1/2-spin Ising model H=0 similar to phase diagrams of fluids.

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Presentation on theme: "S = +1s = -1. Phase diagrams of the 1/2-spin Ising model H=0 similar to phase diagrams of fluids."— Presentation transcript:

1 s = +1s = -1

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5 Phase diagrams of the 1/2-spin Ising model H=0 similar to phase diagrams of fluids

6 EJERCICIO 9: except for T < T c

7 sisi (1944)

8 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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13 rama metaestable región inestable DOMINIOS MAGNÉTICOS

14 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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17 ordered

18 (J>0)

19 EJERCICIO 10 study the nature of the transition for |H| small

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22 EJERCICIO 11a

23 EJERCICIO 11b

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26 Stirling's approx.

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28 Types of boundary conditions:

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32 diverges but only at T=0

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37 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

38 NaF/AlF 3 mixture

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40 structure of  -brass, CuZn

41 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:

42 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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