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Statistical Mechanics - Physics at Oregon State University

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202 CHAPTER 9. GENERAL METHODS: CRITICAL EXPONENTS.<br />

−0.996<br />

−0.998<br />

−1.0<br />

−1.002<br />

−1.004<br />

0.9<br />

0.95<br />

Figure 9.2: Ideal case to find critical exponent.<br />

−1.25<br />

−1.275<br />

−1.3<br />

−1.325<br />

−1.35<br />

0.9<br />

0.95<br />

Figure 9.3: Non-analytic case to find critical exponent.<br />

sample. Hence the procedure to find the critical exponents needs to consider<br />

critical behavior close to the phase transition as a function of sample size. If<br />

we replace the outside of the sample by something else, the values right <strong>at</strong><br />

the critical temper<strong>at</strong>ure change. For example, if we replace the outside by an<br />

effective medium we obtain mean field results right <strong>at</strong> Tc. But away from the<br />

critical temper<strong>at</strong>ure we get the characteristics of the sample, and the outside<br />

world does not play a role. For a finite sample there are no singularities <strong>at</strong> the<br />

phase transition, only smooth changes in behavior. If these changes become<br />

abrupt for in the thermodynamic limit, then we have a singularity and a phase<br />

transition.<br />

x<br />

1.0<br />

x<br />

1.0<br />

1.05<br />

1.05<br />

1.1<br />

1.1

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