Manuscript IV-B@1 · IV-B-v1.tex · lemma · dfb66408

Lemma: Separate spectral estimates

Model 2: dense TT completion and fixed-number spectral removal › Four legs and the distinction between coefficient norms · lines 861–923 · proof included or linked

IV-B@1#lem:spectral, IV-B@1#eq:spectral, IV-B@1#eq:master

Back to manuscript

The pair coefficient is Hilbert–Schmidt and the mixed coefficient is bounded. There are constants independent of the admitted masks such that

Proof. Write ,

Spatial integration by parts and one temporal integration by parts, retaining the initial endpoint , give

For , transversality gives . After absorbing polynomial transfer factors into the arbitrary spatial decay,

For pair signs this implies, after increasing ,

The radial integral is finite. The gravitational low and high tails have squared integrals and . The scalar high tail is , by splitting from and transferring weights between . This proves the first estimate.

For mixed signs, (eq:master) gives

and, on , also the bound with . The low part is Hilbert–Schmidt, with low-tail norm . The two high-tail Schur integrals are , using the appropriate - or -weighted bound; the remaining low-, high- term decays faster. The Schur test proves the second estimate.

Displayed formulas in this passage

  • IV-B@1#eq:spectral · line 866

  • IV-B@1#eq:master · line 889

  • unlabeled · line 876

  • unlabeled · line 882

  • unlabeled · line 898

  • unlabeled · line 910

Nearby in this section