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Notes

Theorem D — Metastability

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  1. #1

    Step 1 (Restricted chain). Define the restricted sub-stochastic matrix on :

    PF(i,j):=Wt(i,j)dt(i)(i,jF),P~F:=12(IF+PF).P_F(i,j):=\frac{W_t(i,j)}{d_t(i)}\quad(i,j\in F),\qquad\tilde P_F:=\tfrac{1}{2}(I|_F+P_F).
  2. #2

    Step 2 (Conductance bound). The conductance of the restricted chain on (with absorbing boundary) is:

    ΦF:=minSFiSjFSP~F(i,j)πF(i)+iSrF,t(i)2πF(i)πF(S)\Phi_F:=\min_{\emptyset\ne S\subsetneq F}\frac{\sum_{i\in S}\sum_{j\in F\setminus S}\tilde P_F(i,j)\pi_F(i)+\sum_{i\in S}\frac{r_{F,t}(i)}{2}\pi_F(i)}{\pi_F(S)}
  3. #3

    The numerator's first term is the internal flow out of within ; the second term is the leakage from to the exterior. Consider the cut of within the full graph. For any :

    iSjSPt(i,j)πF(i)=cutt(S,VS)volt(F)volt(S).\sum_{i\in S}\sum_{j\notin S}P_t(i,j)\pi_F(i) = \frac{\mathrm{cut}_t(S,V\setminus S)}{\mathrm{vol}_t(F)}\cdot\mathrm{vol}_t(S).
  4. #4

    In the worst case (taking to be itself with absorbing exterior), the effective conductance is bounded by . More precisely, for any with :

    ΦF(S)cutt(S,Sˉ)volt(S)ϕt(S).\Phi_F(S)\le\frac{\mathrm{cut}_t(S,\bar S)}{\mathrm{vol}_t(S)}\le\phi_t(S).
  5. #5

    Step 4 (Escape time). The expected absorption time from the quasi-stationary distribution satisfies (see Aldous–Fill, Theorem 12.4; or Montenegro–Tetali, Theorem 3.3):

    EπF[Tesc]12γ~F12θ.\mathbb{E}_{\pi_F}[T_{\mathrm{esc}}]\ge\frac{1}{2\tilde\gamma_F}\ge\frac{1}{2\theta}.