Chapter 11: Observables in Phase Transition Flashcards

1
Q

First-Order Phase Transition

A

discontinuity in the order parameter

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2
Q

Second-Order Phase Transition

A
  • critical singularity can be described by critical exponent with respect to t = |1 - T/TC|
    • universality class: important here; relevant parameters
      • spatial dimensionality D
      • symmetry of order parameter
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3
Q

Specific Heat, Magnetization, and Magnetic Susceptibility

A
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4
Q

Correlation Function

A
  • correlation length diverges as TTC
    • details of lattice and short-range behavior become irrelavant → reason for universality
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5
Q

Scaling and Hyperscaling

A
  • there exist only 2 independent critical exponents
    • there exist scaling relationships between critical exponents
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6
Q

Finite-Size Scaling Theory

(Overview)

A
  • L finite → Z is infinitely differentiable analytic power series → no singularities possible
  • maxima are rounded and displaced
    • max{ζ} ~= L
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7
Q

Finite-Size Scaling Theory

(Assumptions)

A
  • consider susceptibility (below)
  • actually measure scaling function in simulation
    • should get same results regardless of choice of L
    • allows for extrapolation of γ/ν, 1/ν, Tc
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8
Q

Critical Slowing-Down

A
  • correlation time τ for loval MC algorithm given below
    • Recall: Neff = N/(2τ)
    • as L increases, τ increases faster, meaning much longer time is needed to each the same level of accuracy
  • can overcome by using clust algorithms (e.g. Wolff algorithm)
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