Stochastic partial differential equations (SPDEs) play a crucial role in modeling complex surface growth phenomena where randomness and noise are inherent aspects of the system. These equations extend traditional partial differential equations (PDEs) by incorporating stochastic processes, making them ideal for describing surface evolution under random influences like particle deposition, temperature fluctuations, or environmental noise. Below is a detailed exploration of SPDEs in surface growth models.
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Code snippets,MATLAB,7
MATLAB,KPZ Model,1
MATLAB,EW Model,1
MATLAB,MH Model,1
MATLAB,noise in SPDEs,1
MATLAB,Finite Difference methods for SPDEs,1
MATLAB,Monte Carlo Simulations,1
MATLAB,Spectral Methods,1
Code snippets,Python,6
Python,KPZ Model,1
Python,EW Model,1
Python,MH Model,1
Python,noise in SPDEs,1
Python,Finite Difference methods for SPDEs,1
Python,Monte Carlo Simulations,1
Python,Spectral Methods,1
Code snippets,Julia,5
Julia,EW Model,1
Julia,MH Model,1
Julia,noise in SPDEs,1
Julia,Finite Difference methods for SPDEs,1
Julia,Monte Carlo Simulations,1
Code snippets,R,1
R,KPZ Model,1
Code snippets,C++,1
C++,KPZ Model,1
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Code snippets to a typical SPDE used in surface growth
Code snippets to Edwards–Wilkinson (EW) Model
Code snippets to Mullins–Herring (MH) Model
Code snippets to Noise in SPDEs
Finite Difference Methods for SPDEs with code snippets
Monte Carlo Simulations for SPDEs with codes
Spectral Methods for SPDEs with codes
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Ref.,surface growth models,1
Ref.,Euclidean quantum field theories,1
Ref.,fluid dynamics,2
Ref.,stochastic evolution models of biological or chemical quantities,2
Ref.,interest-rate models,2
Ref.,stochastic filtering,3
Ref.,stochastic partial differential equations,9
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Stochastic partial differential equations in Euclidean quantum field theories
Stochastic partial differential equations in fluid dynamics
Stochastic evolution models of biological or chemical quantities
Stochastic evolution models of interest-rate models
Stochastic evolution models of stochastic filtering
Stochastic partial differential equations
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Ref.,Galerkin methods,4
Ref.,physics-informed neural networks,1
Ref.,Fourier neural operators for parameteric PDEs,1
Ref.,deep neural networks,5
Ref.,neural SPDEs,1
Ref.,learning PDEs,3
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Spatial discretizations based on Galerkin methods
Physics-informed neural networks to the solution of SPDEs
Fourier neural operators for parameteric PDEs
Fourier neural operators for deep neural networks
Fourier neural operators for neural SPDEs
The neural network applications for learning PDEs
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Ref.,the universal approximation property of neural networks,7
Ref.,random neural networks,6
Ref.,the Malliavin regularity,2
Ref.,the Stroock-Taylor formula,1
Ref.,the approximation rates for deterministic/random neural networks,2
Ref.,neural networks in the Wiener chaos expansion,10
Ref.,a system of coupled PDEs,5
Ref.,Fourier approaches,2
Ref.,Zakai equation in filtering,4
Ref.,the Adam algorithm,1
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The approximation rates for deterministic/random neural networks
Learn the solution of (SPDE) with (possibly random)neural networks in the Wiener chaos expansion
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Ref.,Jensen's inequality,1
Ref.,the vector-valued Stone-Weierstrass theorem,1
Ref.,Ito's isometry,1
Ref.,isonormal process,1
Ref.,the Wick polynomials,1
Ref.,the Stroock-Taylor formula,1
Ref.,Malliavin calculus for Hilbert space-valued random variables,4
Ref.,the chain rule for the Malliavin derivative,1
Ref.,the Malliavin derivative of a time integral,1
Ref.,the Malliavin derivative of a stochastic integral with F-predictable integrand ,1
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The vector-valued Stone-Weierstrass theorem
Malliavin calculus for Hilbert space-valued random variables
the chain rule for the Malliavin derivative
the Malliavin derivative of a time integral
the Malliavin derivative of a stochastic integral with F-predictable integrand
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