Definition 4.6 (Fruit set).
Ft:={F⊂V:F is a fruit at time t}.
4.5 Basic Properties of Fruits
Proposition 4.7 (Properties).
(i) ∣Ft∣≤2n (finite).
(ii) Ft is gauge-invariant (Lemma 4.3(iv)).
(iii) V∈/Ft, ∅∈/Ft (by (F1)).
(iv) Fruits may overlap: F1∩F2=∅ is possible.
(v) F∈Ft does not imply Fˉ∈Ft.
Proof. (i)--(iii) immediate. (iv) Consider three dense clusters with pairwise overlap. (v) If volt(Fˉ)>21volt(V), then Fˉ violates (F1). □
4.6 Connectivity of Fruits
Definition 4.8 (Minimal fruit).
A fruit F is minimal if no proper non-empty subset of F is itself a fruit.
Lemma 4.9 (Connectivity of minimal fruits). [Corrected]
Every minimal fruit is connected in the induced subgraph Gt[F].
Proof.
Suppose F is a minimal fruit and F=F1⊔F2 is a non-trivial partition with no edges between F1 and F2 inside F. We derive a contradiction.
Step 1. Since there are no internal edges between F1 and F2:
cutt(F,Fˉ)=cutt(F1,Fˉ)+cutt(F2,Fˉ)
and in particular, for each component Fk (k=1,2):
cutt(Fk,Fkˉ)=cutt(Fk,V∖Fk)=cutt(Fk,Fˉ)+0
(the zero comes from no F1--F2 edges). So:
cutt(Fk,Fkˉ)=cutt(Fk,Fˉ).
Step 2 (Both components satisfy (F2)). We show that bothF1 and F2 satisfy the energy ratio condition (F2). From Theorem A (energy isolation), the internal energy of F satisfies:
i,j∈F∑Wt(i,j)≥(1−θ)volt(F).
Since F1 and F2 are disconnected within F, the internal energy of F decomposes exactly:
Step 3 (At least one component satisfies (F1)). Since volt(F)=volt(F1)+volt(F2) and both volumes are positive, at least one component---say F1---satisfies volt(F1)≤21volt(F)≤21volt(V), which is condition (F1).
Conclusion. By Step 2, F1 satisfies (F2). By Step 3, F1 satisfies (F1). Therefore:
ϕt(F1)=volt(F1)cutt(F1,F1ˉ)≤θ.
So F1 is a fruit---contradicting the minimality of F. □
Corollary 4.10 (Connectivity of general fruits).
Every fruit contains a connected sub-fruit. In particular, every "meaningful" (minimal) fruit is connected.
Proof. Any fruit either is minimal (hence connected by Lemma 4.9) or contains a proper sub-fruit. Iterating produces a minimal sub-fruit, which is connected. □
4.7 Spectral Characterisation
Definition 4.11 (Normalised Laplacian).
Lt:=I−Dt−1/2AtDt−1/2
where Dt=diag(dt(i)) and (At)ij=Wt(i,j).
Eigenvalues: 0=λ1≤λ2≤⋯≤λn.
Discrete Cheeger Inequality
Theorem 4.12 (Discrete Cheeger inequality; Fact B.3).
For the Cheeger constant ht:=min∅=S⊊Vϕt(S):
2λ2≤ht≤2λ2.
Proof sketch.
Lower bound (λ2≤2ht). Use the variational characterisation of λ2 and test with the normalised indicator of any set S:
Then fS⊥Dt1/21 and the Rayleigh quotient satisfies R(fS)≤2ϕt(S).
Upper bound (ht≤2λ2). Sweep the level sets of the second eigenvector f2 and apply the discrete coarea inequality (Alon--Milman). □
Spectral Approximation
Corollary 4.13 (Spectral signature of fruits).
If a fruit F exists with ϕt(F)≤θ, then λk≤2θ for some k, and the normalised indicator of F is approximated to O(θ) accuracy by a linear combination of the first k eigenvectors.
Proof sketch. The Rayleigh quotient of F's indicator is ≤2θ. By min-max, λk≤2θ for some k. Davis--Kahan's sinΘ theorem (Fact B.4) bounds the angle. □
4.8 Energy Isolation (Theorem A)
Theorem A (Energy isolation).
For any fruit F∈Ft:
volt(F)∑i,j∈FWt(i,j)≥1−θ.
Proof.
Step 1. Volume decomposition:
volt(F)=i,j∈F∑Wt(i,j)+cutt(F,Fˉ).
Step 2. By (F2), ϕt(F)≤θ. By (F1), volt(F)=min{volt(F),volt(Fˉ)}. Thus:
cutt(F,Fˉ)=ϕt(F)⋅volt(F)≤θ⋅volt(F).
Step 3.i,j∈F∑Wt(i,j)=volt(F)−cutt(F,Fˉ)≥(1−θ)volt(F). Divide by volt(F)>0. □
Sharpness. Equality holds when ϕt(F)=θ and volt(F)=21volt(V).
Theorem D (Metastability).
Let X0∼πF (the stationary distribution restricted to F). The escape time from F under P~t satisfies:
E[Tesc(F)]≥2θ1.
Proof.
Step 1. Define the restricted sub-stochastic matrix PF(i,j):=Wt(i,j)/dt(i) for i,j∈F (zero otherwise). Row sums are 1−rF,t(i)<1 (leakage). The lazy version is P~F:=21(I∣F+PF).
Step 2. Let ΦF denote the conductance of P~F viewed as a chain on F with absorbing boundary. By the Sinclair--Jerrum bound (Fact B.6), the spectral gap satisfies γF≤2ΦF.
Step 3. The internal conductance ΦF is bounded by the external conductance: ΦF≤ϕt(F)≤θ. This is because any internal cut S⊊F either has the same cut value as a cut of V (contributing to ϕt(F)), or the absorbing boundary provides additional "leakage" but does not reduce conductance.
Step 4. For the lazy chain, the spectral gap is γ~F=γF/2≤θ.
Step 5. The expected absorption time (escape time) from the stationary distribution satisfies the standard bound (see Levin--Peres--Wilmer, Theorem 12.4):
EπF[Tesc]≥2γ~F1≥2θ1.□
Interpretation. A random walk starting inside a fruit remains trapped for Ω(1/θ) steps. For θ=0.05, the expected escape time is at least 10 steps.