Manuscript XIX-A@1 · XIX-A.tex · lemma · e30d8062
Lemma: Existence and uniqueness of the displayed prescription
The finite-time harmonic relational scalar › An explicit comparison prescription · lines 344–385 · proof included or linked
XIX-A@1#lem:harmonic-existence
Equations (eq:W1)–(eq:W2) with (eq:harmonic-data) have unique smooth coefficient fields. Uniqueness does not require spatial decay of the compared smooth solutions.
Proof. For a smooth spatially compact forcing , the solution of with zero coordinate-time data is
The quotient has its continuous value at zero frequency. Spatial Fourier transformation verifies the equation and data. Smoothness follows by differentiating the Fourier integral, or by the standard local wave estimates. Apply this construction first to (eq:W1), and then to (eq:W2). The second forcing is spatially compact because are.
For uniqueness, let be a smooth homogeneous solution with zero data. On a shrinking ball of radius , its wave energy
has nonpositive derivative. The boundary flux is
Since , the solution vanishes on the corresponding interior cone. Taking large enough treats any chosen point. The argument is local and imposes no condition at spatial infinity. Apply it successively to the differences of the first and second coefficient solutions.
Displayed formulas in this passage
unlabeled · line 355
unlabeled · line 370
unlabeled · line 375