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Euler has state error but exact log-density quadrature for a linear flow

Example

Assume Countable Choice. Let f(t,x)=x on [0,1]×R, start at x(0)=1, take h=1/N, and use any strictly positive continuous probability density p0 on R. Initialize ℓ^0=log⁡p0(1). The exact state is x(t)=et, while Euler gives xn=(1+h)n, so its final state error is e−(1+1/N)N>0. The exact continuous-flow log-density change is −1, and the Euler divergence accumulator also gives exactly −1.

Facts & Assumptions

Given: Countable Choice, T=1, N≥1, h=1/N, f(t,x)=x on [0,1]×R, x(0)=1, a positive continuous probability density p0 on R, and the Euler state and divergence updates initialized by ℓ^0=log⁡p0(1).

[A1]

Countable Choice is the assertion that every countable family of nonempty sets has a choice function (The Axiom of Countable Choice (ACω)); it is used only for the density interpretation inherited from [F1].

[F1]

For a C¹ diffeomorphic flow, pt(Φt(x0))=p0(x0)/det⁡DΦt(x0) and the log-density derivative is −div⁡f (A continuous flow changes log density by minus its divergence).

[F2]

Under the stated C² tube and flow hypotheses, Euler state updates and the divergence accumulator have the fixed-time error bounds proved in Euler global state and log-density error on a bounded C² tube.

[F3]

The real exponential is defined by its power series, is differentiable with derivative exp⁡, and satisfies exp⁡(0)=1 (The real exponential function and the number e by a power series, The exponential function is smooth and (exp⁡)′=exp⁡).

[F4]

exp⁡(t)>0 and 1/exp⁡(t)=exp⁡(−t) (The exponential is positive and satisfies exp⁡(−x)=1/exp⁡(x)).

[F6]

exp⁡ is strictly increasing (The exponential function is strictly increasing).

[F7]
[F8]

Natural powers preserve order on nonnegative bases for exponent N≥1 (Monotonicity of x↦xn and of n↦an); they satisfy the recursive natural-power definition (Integer powers am).

[F10]

For positive u,v, log⁡(u/v)=log⁡u−log⁡v (Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm).

[F11]

The natural logarithm is the inverse of exp⁡ on positive reals, so log⁡(exp⁡u)=u (The natural logarithm as the inverse of the exponential function).

Verification

1.1givenF2F3F4F5F6F7F8F9inductionalgebra

Extend the given field to the open domain R2 by the same formula f(t,x)=x; its restriction to [0,1]×R is unchanged. Define Φt(x0):=exp⁡(t)x0 for t∈[0,1]. By [F3] and [F9], ∂tΦt(x0)=exp⁡(t)x0=f(t,Φt(x0)) and Φ0(x0)=x0; [F4] makes every slice a C¹ diffeomorphism R→R with inverse y↦y/exp⁡(t). Thus x(t)=Φt(1)=exp⁡(t) is the exact path. Euler satisfies xn+1=(1+h)xn, so induction gives xn=(1+h)n. Since h>0, [F5] gives exp⁡(h)−1=exp⁡(c)h for some c∈(0,h), and [F6] with exp⁡(0)=1 gives exp⁡(c)>1, hence 1+h<exp⁡(h). By [F8], (1+h)N<exp⁡(h)N; [F7] gives exp⁡(h)N=exp⁡(Nh)=exp⁡(1), so ∣xN−x(1)∣=exp⁡(1)−(1+h)N>0. For 1≤n≤N, [F8] and [F7] give 1≤xn≤exp⁡(nh)≤exp⁡(1), while x0=1; exact states lie in [1,exp⁡(1)] by [F6]. Therefore K=[0,exp⁡(1)] contains the exact path and Euler nodes. The bounded convex open set U=(−1,2)×(−1,exp⁡(1)+1) contains [0,1]×K, and f(t,x)=x is C² with bounded derivatives there, so [F2] applies.

2.1givenA1F1F4F10F11step 1.1algebra∎

Here DΦ1(1)=exp⁡(1), so [F1] gives p1(exp⁡(1))/p0(1)=1/exp⁡(1)=exp⁡(−1) by [F4]. Since p0(1)>0, [F10] and [F11] show that the exact log-density change is log⁡(p1(exp⁡(1)))−log⁡p0(1)=−1. Euler subtracts hdiv⁡xf=h on each of the N steps, so its computed change is −Nh=−1; with the given exact initialization, the log-density error is zero despite the positive state error from step 1.1.

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