In mathematics, the infinity Laplace (or L ∞ {\displaystyle L^{\infty }} -Laplace) operator is a 2nd-order partial differential operator, commonly abbreviated Δ ∞ {\displaystyle \Delta _{\infty }} . It is alternately defined, for a function u : R n ⟶ R {\displaystyle u:\mathbb {R} ^{n}\longrightarrow \mathbb {R} } of the variables x = ( x 1 , … , x n ) {\displaystyle x=(x_{1},\dots ,x_{n})} , by
Δ ∞ u = ⟨ D u , D 2 u D u ⟩ = ∑ i , j = 1 n ∂ 2 u ∂ x i ∂ x j ∂ u ∂ x i ∂ u ∂ x j {\displaystyle \Delta _{\infty }u=\langle Du,D^{2}u\,Du\rangle =\sum _{i,j=1}^{n}{\frac {\partial ^{2}u}{\partial x_{i}\,\partial x_{j}}}{\frac {\partial u}{\partial x_{i}}}{\frac {\partial u}{\partial x_{j}}}}
or
Δ ∞ u = ⟨ D u , D 2 u D u ⟩ | D u | 2 = 1 | D u | 2 ∑ i , j = 1 n ∂ 2 u ∂ x i ∂ x j ∂ u ∂ x i ∂ u ∂ x j , {\displaystyle \Delta _{\infty }u={\frac {\langle Du,D^{2}u\,Du\rangle }{|Du|^{2}}}={\frac {1}{|Du|^{2}}}\sum _{i,j=1}^{n}{\frac {\partial ^{2}u}{\partial x_{i}\,\partial x_{j}}}{\frac {\partial u}{\partial x_{i}}}{\frac {\partial u}{\partial x_{j}}},}
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