Split-Step Methods for Fully Stiff Problems
When both drift and diffusion terms are stiff, split-step methods treat both parts implicitly. These methods can handle the most challenging stiff SDE problems.
Split-Step Implicit Methods
ISSEM - Implicit Split-Step Euler-Maruyama
ISSEulerHeun - Implicit Split-Step Euler-Heun
When to Use Split-Step Methods
Use ISSEM when:
- Both drift and diffusion are stiff
- Explicit methods fail even with small time steps
- Standard implicit methods (ImplicitEM) are insufficient
- Working with Itô interpretation
Use ISSEulerHeun when:
- Both drift and diffusion are stiff
- Working with Stratonovich interpretation
- Need implicit treatment of diffusion term
Understanding Full Stiffness
Drift Stiffness: Large negative eigenvalues in f(u,t) Diffusion Stiffness: Large coefficients in g(u,t) causing instability
Detection Signs:
- ImplicitEM still requires very small time steps
- Solutions become unstable despite implicit drift treatment
- Large diffusion coefficients cause numerical artifacts
Algorithm Structure
Split-step methods solve:
du = f(u,t)dt + g(u,t)dW
By treating both terms implicitly through operator splitting or fully implicit schemes.
Performance Considerations
- More expensive per step than drift-only implicit methods
- May require smaller time steps than expected
- Jacobian computations for both drift and diffusion
- Nonlinear solve complexity increases
Configuration
Same options as other implicit methods:
ISSEM(
linsolve = KrylovJL_GMRES(),
nlsolve = NLNewton(),
theta = 1.0,
autodiff = true
)
Alternative Approaches
If split-step methods are too expensive:
- Try stabilized explicit methods (SROCK family)
- Consider method of lines for PDE problems
- Use shorter time intervals with restarts
- Reformulate problem to reduce stiffness
References
- Implicit-explicit splitting schemes for SDEs
- Stochastic operator splitting methods