Infinite-dimensional operator ridgelet transform

4. Tempered synthesis activations and ReLU🔗

This chapter is Section 5 of the manuscript together with Appendix C. The analysis filter \rho is a Schwartz function, but the activation that synthesizes a network may be unbounded; a real \beta\in\mathcal S'(\mathbb R) is paired with the band-pass filter through the distributional constant C_{\beta,\rho}^{(\alpha)}=\frac1{2\pi}\langle\widehat\beta,\widehat\rho(-\,\cdot\,)|\cdot|^{-\alpha}\rangle of Definition 3.1.4, which is well defined because \widehat\rho vanishes near the origin. The weighted Sobolev activation spaces \mathcal A_{s,t}=\langle\cdot\rangle^tH^s(\mathbb R), in which this pairing is continuous, are recalled from Appendix C.

  1. 4.1. Regularized synthesis
  2. 4.2. Weighted Sobolev activation spaces and standard activations
  3. 4.3. Weak Sobolev regularity along rays
  4. 4.4. Non-band-pass filters for Sobolev synthesis