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Distributional equation convention for complex Schrödinger solutions

Definition

Let Q⊆R1+n be open, with n≥1; its first coordinate is time t and the remaining coordinates are space x=(x1,…,xn). A test function on Q is a complex-valued smooth function with compact support in Q; write D(Q)=Cc∞(Q;C) and equip it with the test-function topology. A complex distribution on Q is a continuous complex-linear functional on D(Q); its value on η is written ⟨u,η⟩. The pairing is linear in both entries, with no conjugation of the test function. The space of these functionals is D′(Q).

For a multi-index α in the space-time coordinates, the distributional derivative is defined by ⟨∂αu,η⟩=(−1)∣α∣⟨u,∂αη⟩. Here ∣α∣ is the sum of the entries of α. The spatial Laplacian is Δxu=∑j=1n∂xj2u.

If u,F∈D′(Q), the equation i∂tu+Δxu=F holds in distributions on Q precisely when ⟨i∂tu+Δxu,η⟩=⟨F,η⟩ for every η∈D(Q). The same convention applies to an equation with additional terms, provided each term has independently been specified as a distribution. In particular, a nonlinear expression is included only when the chosen solution class makes it a distribution.

This interior space-time identity asserts neither existence of an initial value or boundary trace nor any regularity or local integrability of a nonlinear expression. Such properties and conditions require separate hypotheses. The bilinear distribution pairing is distinct from any conjugated Hilbert-space or antidual pairing.

Justification

The test functions and their topology give the domain of the continuous linear functionals in Distribution. By Distributional derivative, each specified derivative is again a distribution; finite sums and scalar multiples of distributions are distributions. Consequently both sides of the displayed equation are functionals on the same test space, and equality on every test function is a well-defined equality in D′(Q). This construction does not establish that a proposed nonlinear expression defines a distribution.

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