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The following argument summarizes the convergence theory for inexact inner iterations. First, we provide an expression for the error in the linear system during the inner iterations. Then we derive a monotonic bound on the error during the outer iterations. Let g( j) = y( j) − x be the error after the jth inner iteration. Lemma 16. In the inner-outer iteration with 0 < α < 1 and β < α, when the inner iterations are solved using a Richardson iteration, after j inner iterations, ⎛ α−βj−1 ⎞ g(j) =y(j)−x= αβj−1Pj +( )∑βlPl g(0) j≥1, where g(0) = y(0) − x = x(k) − x is the error after the kth outer iteration. ⎝ βl=1⎠ Proof. We proceed by induction. In the base case, g(1) = αPg(0) follows because one inner iteration is identical to an iteration of the power method. Consider g( j+1). First, expand g( j+1) = βPy( j) + (α − β)Px(k) + (1 − α)v − x = βPg( j) + (α − β)Pg(0) . Now apply the induction hypothesis and simplify: ⎛ α−βj−1 ⎞ g(j+1)=βP (αβj−1Pj+ )∑βlPl g(0)+(α−β)Pg(0) = = ⎝ βl=1⎠ ⎛ j−1⎞ αβjPj+1 +(α−β)P+(α−β)∑βlPl+1 g(0) ⎝ l=1⎠ ⎛α−βj⎞ αβjPj+1 +( )∑βlPl ⎝ βl=1⎠ g(0). We know that ∥g(1)∥ ≤ α ∥g(0)∥ because it’s just a step of the power method, and the above equation says the same thing. The next iterate satisfies ∥g(2)∥ = ∥αβP2g(0) + (α − β)Pg(0)∥ ≤ αβ ∥g(0)∥ + (α − β) ∥g(0)∥ = ((α − 1)β + α) ∥g(0)∥ ≤ α ∥g(0)∥ , (5.11) (5.12) (5.13) (5.14) and so we monotonically decrease a bound on the error for the first two iterations. 5.4 ⋅ convergence 99PDF Image | MODELS AND ALGORITHMS FOR PAGERANK SENSITIVITY
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