An optimal variance estimate in stochastic homogenization of discrete elliptic equations

By Antoine Gloria, Felix Otto. 2011

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We consider a discrete elliptic equation with random coefficients $A$, which (to fix ideas) are identically distributed and independent from grid point to grid point $x\in\mathbb{Z}^d$. On scales large w.\ r.\ t.\ the grid size (i.\ e.\ unity), the solution operator is known to behave like the solution operator of a (continuous) elliptic equation with constant deterministic coefficients. These symmetric ''homogenized'' coefficients $A_{hom}$ are characterized by % $$ \xi\cdot A_{hom}\xi\;=\;\langle\left((\xi+\nabla\phi)\cdot A(\xi+\nabla\phi)\right)(0)\rangle, \quad\xi\in\mathbb{R}^d, $$ % where the random field $\phi$ is the unique stationary solution of the ''corrector problem'' % $$ -\nabla\cdot A(\xi+\nabla\phi)\;=\;0 $$ % and $\langle\cdot\rangle$ denotes the ensemble average. \medskip It is known (''by ergodicity'') that the above ensemble average of the energy density $e=(\xi+\nabla\phi)\cdot A(\xi+\nabla\phi)$, which is a stationary random field, can be recovered by a system average. We quantify this by proving that the variance of a spatial average of $e$ on length scales $L$ is estimated as follows: % $$ {\rm var}\left[\sum_{x\in\mathbb{Z}^d}\eta_L(x)\,e(x)\right] \;\lesssim\;L^{-d}, $$ % where the averaging function (i.\ e.\ $\sum_{x\in\mathbb{Z}^d}\eta_L(x)=1$, ${\rm supp}\eta_L\subset[-L,L]^d$) has to be smooth in the sense that $|\nabla\eta_L|\lesssim L^{-1}$. In two space dimensions (i.\ e.\ $d=2$), there is a logarithmic correction. \medskip In other words, smooth averages of the energy density $e$ behave like as if $e$ would be independent from grid point to grid point (which it is not for $d>1$). This result is of practical significance, since it allows to estimate the error when numerically computing $A_{hom}$.

Subfields: Applied Mathematics, Computational Theory and Mathematics, Mechanics of Materials

View Paper: https://www.semanticscholar.org/paper/e98e3c63dcb6cb2bb021a89dd954eeb40015c31a

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In Applied Mathematics

  1. S. Armstrong
  2. Jean-Christophe Mourrat
  3. Tuomo Kuusi
  4. Felix Otto
  5. Stefan Neukamm
  6. Antoine Gloria
  7. Zhongwei Shen
  8. Charles K. Smart

In Computational Theory and Mathematics

  1. S. Armstrong
  2. Jean-Christophe Mourrat
  3. Felix Otto
  4. Tuomo Kuusi
  5. Antoine Gloria
  6. Stefan Neukamm
  7. Zhongwei Shen
  8. Charles K. Smart

In Mechanics of Materials

  1. S. Armstrong
  2. Jean-Christophe Mourrat
  3. Felix Otto
  4. Stefan Neukamm
  5. Tuomo Kuusi
  6. Antoine Gloria
  7. Zhongwei Shen
  8. Charles K. Smart

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