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--- title: "Newton's Method" source: https://www.jemoka.com/posts/kbhnewton_s_method/ --- constituents requirements A Newton step is: \begin{align} \Delta x_{nt} = -\nabla^{2}f\qty(x)^{-1}\nabla f\qty(x) \end{align} additional information Newton’s method is affine invariant! convergence Then number of steps until convergence for Newton’s method relates to the third derivative because its step changes as a function of how the second derivative changes. Number of iterations until \(f\qty(x) - p^{*} \leq \epsilon\) is bounded above by: \begin{align} \frac{f\qty(x^{(0)}) - p^{*}}{\gamma} + \log \log \qty(\frac{\epsilon_{0}}{\epsilon}) \end{align} \(\gamma\), \(\epsilon_{0}\) that depends on the strong convexity constant and the Lipschitz Constant etc. You basically never knows the constants so give up. oh also you need to know \(p^{*}\). Newton’s decrement \begin{align} \lambda \qty(x) = \qty(\nabla f\qty(x)^{T} \nabla^{2}f\qty(x)^{-1} \nabla f\qty(x))^{\frac{1}{2}} \end{align} which is a measurement between the distance between \(x\) and \(x^{*}\). implementing Newton’s Method Two basic steps: form a Hessian solve it. We can evaluate derivatives and solve the Newtonian system: \begin{align} H\Delta x = -g \end{align} where \(H = \nabla^{2} f\qty(x), g = \nabla f\qty(x)\). We naively would solve with Cholesky factorization: \(H = LL\) \(\Delta x_{nt} = -L^{-T} L^{-1} g\) \(\lambda \qty(x) = \norm{L^{-1}g}_{2}\) we can thus exploit the structures as needed. 205L Notation \begin{equation} f(x) \approx f(x_{t-1}) + (x-x_{t-1}) f’(x_{t-1}) + \frac{(x-x_{t-1})^{2}}{2} f’’(x_{t-1}) \end{equation} Taking a derivative with respect to this, we obtain: \begin{equation} f’(x_{t-1}) + (x-x_{t-1}) f’’(x_{t-1}) \end{equation} Solving the update equation for zero, we obtain that: \begin{equation} x = x_{t-1} - \frac{f’(x_{t-1})}{f’’(x_{t-1})} \end{equation} This converges quadratically!! to solve for minima/maxima. For solving minima/maxima for gardients: \begin{equation} x_{t} = x_{t-1} - \qty(\bold{H}_{g})^{-1}\nabla J \end{equation} for Hessian \(H\) and gradient \(g\). For finding ZEROS instead of minima: \begin{equation} x = x_{t-1} - \frac{f(x_{t-1})}{f’(x_{t-1})} \end{equation} graphical intuition We want to drop down a tangent line from the standing point until we hit \(0\), and then go to that point on the function and draw a tangent line again. Namely, we write: \begin{equation} f’\qty(x^{(j)}) = \frac{f\qty(\qty(x^{(j)}))}{\delta} \end{equation} for small \(\delta\), Meaning, \(\delta = \frac{f\qty(x^{(j)})}{f’\qty(x^{(j)})}\), which is the gap between each step. Then we update just by this ratio \(x = x - \delta\) Failure Case If the function is near an inflection point (i.e. with bad quadratic approximation), you may converge at a point which doesn’t satisfy SONC (i.e. you will get an inflection but not a minima).