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7.1 Diffusion Monte Carlo (DMC)
First suggested in the forties (see [MEYERS 56]);
rediscovered in the eighties ([CEPERLEY 80]).
Originally applied to the ground state of a bosonic system
such as
He [KALOS 74,WHITLOCK 79].
Later: extended to fermions and excited states
([BARNETT 86,CEPERLEY 88]); see also [CEPERLEY 96].
Time-dependent Schroedinger equation for a particle of mass
in a potential
:
|
(7.1) |
with the energy operator
|
(7.2) |
and a trial energy .
Define an imaginary time variable
; then
|
(7.3) |
with
.
Diffusion with autocatalysis!
Visualize as describing the density of bacteria diffusing in a fluid
with locally varying nutrient concentration.
Expand in eigenfunctions of :
Solve 7.3 for various values of :
find that for which remains stationary. Then
and
.
How to solve 7.3?
Consider the diffusion and the autocatalysis parts of the equation
separately.
Diffusion part:
|
(7.5) |
May be solved by a random walk procedure:
Start Brownian walkers
|
(7.6) |
where are drawn from a Gauss distribution with
.
Now consider an ensemble of such -particle systems and
write the local distribution density at time as
|
(7.7) |
This is an estimate for the solution
of the diffusion equation .
Autocatalysis part:
|
(7.8) |
Instead of writing the formal solution as
|
(7.9) |
we use once more a stochastic method.
Consider an ensemble of systems of particles each, at fixed positions.
Let the number of systems in the ensemble be allowed to vary:
- Systems that contain many particles located at positions with
high values of
are replicated
- Systems with unfavorable configurations are deleted
Procedure:
Let the ensemble be given at step .
Again, the distribution density
7.7 is an estimate of the density at position
.
Combining the two stochastic techniques for solving the
diffusion and autocatalytic equations we obtain the following
procedure.
Figure 7.1:
Quantum mechanical diffusion Monte Carlo
|
So far: must be real and
Bosons
(
He or similar).
Generalization for fermions: fixed node and
released node approximation [CEPERLEY 88].
Note: The analogy between the wave function
and the local density
is purely formal.
It must be distinguished from the physical interpretation of
.
Importance sampling DFT:
If the potential
is highly negative in some region of space,
the autocatalytic term may get out of control and must be handled differently:
- Introduce an estimate
of the correct solution
;
- define an auxiliary function
|
(7.11) |
- insert this in 7.3 to find
|
(7.12) |
Since
|
(7.13) |
the autocatalytic term is now well-behaved, and the
multiplicity will remain bounded.
Visualisation of equ. 7.12: The new term looks like an
advective contribution. In the image of a diffusing
and multiplying bacterial strain there is now an additional
driving force
|
(7.14) |
which creates a flow, or drift. This means that the
individual diffusors follow a preferred direction along
:
|
(7.15) |
The multiplicity is now
|
(7.16) |
Green's function Monte Carlo (GFMC):
Another formulation of the DMC procedure [SKINNER 85].
Recent literature:
See [CEPERLEY 96] and web sites [CEPERLEY WWW] or [CAVENDISH WWW].
Next: 7.2 Path Integral Monte
Up: 7. Quantum Mechanical Simulation
Previous: 7. Quantum Mechanical Simulation
Franz J. Vesely Oct 2005
See also: "Computational Physics - An Introduction," Kluwer-Plenum 2001