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Marcel Hudiani

Publications and source records attributed to Marcel Hudiani.

2 recordsLinked to original sources

Convergence Rate for the Last Iterate of Stochastic Gradient Descent Schemes

We study the convergence rate for the last iterate of stochastic gradient descent (SGD) and stochastic heavy ball (SHB) in the parametric setting when the objective function $F$ is globally convex or non-convex whose gradient is $\gamma$-H\"{o}lder. Using only discrete Gronwall's inequality without Robbins-Siegmund theorem, we recover results for both SGD and SHB: $\min_{s\leq t} \|\nabla F(w_s)\|^2 = o(t^{p-1})$ for non-convex objectives and $F(w_{\tau \wedge t}) - F_* = o(t^{2\gamma/(1+\gamma) \cdot \max(p-1,-2p+1)-\epsilon})$ for $\beta \in (0, 1)$, $\tau := \inf \{ t > 0 : F(w_t) = F_*\}$, and $\min_{s \leq t} F(w_s) - F_* = o(t^{p-1})$ for convex objectives $F$ whose minimum is $F_*$. In addition, we proved that SHB with constant momentum parameter $\beta \in (0, 1)$ attains a convergence rate of $F(w_t) - F_* = O(t^{\max(p-1,-2p+1)} \log^2 \frac{t}{\delta})$ with probability at least $1-\delta$ when $F$ is convex and $\gamma = 1$ and step size $\alpha_t = \Theta(t^{-p})$ with $p \in (\frac{1}{2}, 1)$.

math.OC

Singular diffusion limit of a tagged particle in zero range processes with Sinai-type random environment

We derive a singular diffusion limit for the position of a tagged particle in zero range interacting particle processes on a one dimensional torus with a Sinai-type random environment via two steps. In the first step, a regularization is introduced by averaging the random environment over an $\varepsilon N$-neighborhood. With respect to such an environment, the microscopic drift of the tagged particle is in form $\frac{1}{N}W_\varepsilon'$, where $W_\varepsilon'$ is a regularized White noise. Scaling diffusively, we find the nonequilibrium limit of the tagged particle $x^\varepsilon_t$ is the unique weak solution of $d x_t^{\varepsilon} = 2\frac{\Phi(\rho^{\varepsilon}(t, x_t^{\varepsilon}))}{\rho^{\varepsilon}(t, x_t^\varepsilon)} \,W_{\varepsilon}'(x_t^\varepsilon) + \sqrt{\frac{\Phi(\rho^{\varepsilon}(t, x_t^\varepsilon))}{\rho^{\varepsilon}(t, x_t^\varepsilon)}} \,dB_t$, in terms of the hydrodynamic mass density $\rho^\varepsilon$ recently identified and homogenized interaction rate $\Phi$. In the second step, we show that $x^\varepsilon$, as $\varepsilon$ vanishes, converges in law to the diffusion $x^0$ described informally by $d x_t^0 = 2\frac{\Phi(\rho^{0}(t, x_t^{0}))}{\rho^{0}(t, x_t^0)} \,W'(x_t^0) + \sqrt{\frac{\Phi(\rho^{0}(t, x_t^0))}{\rho^{0}(t, x_t^0)}} \,dB_t$, where $W'$ is a spatial White noise and $\rho^0$ is the para-controlled limit of $\rho^\varepsilon$ also recently identified, solving the singular PDE $ \partial_t \rho^0 = \frac{1}{2}\Delta \Phi(\rho^0) - 2\nabla \big(W' \Phi(\rho^0)\big)$.

math.PR