StoppedMoments #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The stopped mean and the stopped second moment #
Fix a conservative Feller process with continuous paths, an open set U, a deterministic
horizon t, and a starting point x of U. Write theta for the stopped time
exitTimeTrunc U t, so that the stopped position is omega theta.
Two observables are treated, and both are treated in the same way: an observable compared with
a function reproduced by the exit distribution of U.
The stopped mean. If
uis reproduced by the exit distribution ofU, if|b - u| <= Keverywhere andb x = 0, then|E_x[b(X_theta)]| <= 2K. The two summands are the valueu x, which is withinKofb x = 0, and the expectation ofb - u, which is withinKbecause the law is a probability measure.The stopped second moment. If
u = h - sigma * wwithhreproduced by the exit distribution andwthe expected exit time, if|q - u| <= Keverywhere andq x = 0, then|E_x[q(X_theta)] - sigma * t| <= 2K + sigma * t * P_x[tau <= t]. The second identity of the stopped-Dirichlet file turnsE_x[u(X_theta)]intou x + sigma E_x[theta], and the expected stopped time is the horizon less a shortfall supported on the event that the exit has already occurred.
The two conclusions are the displays e.displacement.squared.stopped and
e.second.moment.stopped of the source, in one direction each: there b is a linear function,
q a quadratic one, sigma is twice the effective diffusivity at the scale of the cube, and
K is the uniform distance between the heterogeneous solution and its homogenized counterpart.
Summing over a family of observables is the last section; it produces the displacement bound
and the second moment of the whole displacement vector, with leading term n * sigma * t over
n directions.
Nothing here refers to a generator, to a coefficient field, or to a cube. The two inputs that
carry the analytic content are HasExitMeanValueOn — the mean-value property of the
observable, supplied by the exit mean-value interface — and the uniform bound K, supplied by
the renormalization of the generator.
Main results #
ae_eval_exitTimeTrunc_mem_closure— the stopped position lies in the closure ofU.integral_eval_exitTimeTrunc_congr_of_eqOn_closure— only the values on the closure matter.abs_integral_eval_exitTimeTrunc_le_of_hasExitMeanValueOn— the stopped mean.abs_integral_eval_exitTimeTrunc_sub_mul_le_of_hasExitMeanValueOn— the stopped second moment.abs_integral_sum_eval_exitTimeTrunc_sub_le— the sum over a family of directions.
References #
- ABK26, Steps 1 and 3 of the superdiffusive displacement bounds of Section 5.4.
1. Two elementary bounds #
2. The stopped position #
The composition of a Borel function with the stopped position is Borel.
A bounded Borel observable of the stopped position is integrable.
The stopped position lies in the closure of the domain. Almost every path of the
process started inside U starts inside U, and a continuous path started inside U is in
the closure of U at the time at which it either leaves U or reaches the horizon.
Only the values on the closure matter. Two observables agreeing on the closure of U
have the same expectation at the stopped position.
3. The shortfall of the stopped time against the horizon #
The shortfall of the stopped time against the horizon is nonnegative.
The shortfall of the stopped time against the horizon is at most the horizon times the probability that the exit has already occurred.
4. Summing over a family of directions #
The second moment of the whole displacement. If a finite family of observables adds up
on the closure of U to a single observable N, and each member is within B of sigma * t
at the stopped position, then N is within n * B of n * sigma * t there.
With N the squared norm and sigma twice the effective diffusivity, the leading term is
n * sigma * t, the source's 2 d shom_m t over the d coordinate directions.
5. The stopped mean #
The stopped mean. Let u be reproduced by the exit distribution of U and let b
be a Borel observable within K of u everywhere and vanishing at the starting point. Then
the expectation of b at the stopped position is at most 2K in absolute value.
This is the display e.displacement.squared.stopped of the source before squaring: b is the
linear function e ⬝ x, u is the heterogeneous solution taking those boundary values, and
K is the uniform distance between them.
6. The stopped second moment #
The stopped second moment. Let h be reproduced by the exit distribution of U, let
u be h corrected by sigma times the expected exit time, and let q be a bounded Borel
observable within K of u everywhere and vanishing at the starting point. Then the
expectation of q at the stopped position is within 2K of sigma times the horizon, up to
the shortfall carried by the event that the exit has already occurred.
This is the display e.second.moment.stopped of the source: q is the quadratic observable
(e ⬝ x)^2, sigma is twice the effective diffusivity at the scale of the cube, u is the
heterogeneous solution with that constant right-hand side and those boundary values, and K
is the uniform distance between u and q.