Sampling theory and why I reject a lot of papers @JoelRosenfeld

Uploaded March 2021 | Updated September 2026, 13 hours ago

Here we demonstrate the Nyquist theorem through reproducing kernel HIlbert spaces, specifically, the Paley Wiener Space

Five Short Stories about Cardinal Series: ams.org/journals/bull/1985-12-01/S0273-0979-1985-15293-0/S0273-0979-1985-15293-0.pdf

Music:
Come 2gether by Ooyy
MIA by R. A. D.
Video Call from Los Angeles by Trevor Kowalski
Into the Blue by the Luwaks
Guardians + Tek by Craig Hardgrove

Thanks to cassandra50 on Reddit for helping me find the scene from the Good Fight.

Sampling theory and why I reject a lot of papers

Tomography - Discrete Fourier Transfroms and Other Discrete Operators

Essential Math for a PhD in the U.S. #phdlife #mathematics

What is a delta function? From distributions to reproducing kernels.

Intro to Operator Theory : Adjoints and Inverses

#BulletTalk - Forced to do this in 3 minutes - Dynamic Mode Decompositions with Liouville Operators

The Bahamas, Occupation Kernels, and System Identification

Numerical Analysis - Final Review Part 2

$The Two Hilbert Spaces (for Nonlocal Operators) Dynamic Mode Decomposition is an operator theoretic approach to the study of dynamical systems. The way it got its start was by looking at high dimensional systems, and stacking the snapshots into a matrix that was decomposed later. The eigendecomposition of this matrix provided Dynamic Modes, which gave the dominant modes of the system. However, this approach is extremely limiting, where you can only have as many samples of your space as you have dimensions before you saturate the rank of the matrix. The led to the use of extended DMD methods, where the states were thrown into a high dimensional feature space. Inevitably, this gave rise to infinite dimensional feature spaces and Koopman operators, which is how the connections with reproducing Kernel Hilbert Spaces first came about. Our work has been towards expanding the scope of Dynamic Mode Decompositions, where our first manuscripts in the field removed the Koopman operator from the analysis, and instead used Liouville operators. By directly accessing these operators, we are removing the requirements that a system is discretizable (forward complete/invariant). But this still leverages operators of functions of the state. To further extend these ideas to include nonlocal operators within their scope, we need to operate on Hilbert Spaces composed of functions that send continuous signals or trajectories to signals and trajectories. By introducing spaces like these, we can now look at operators that are nonlocal, which includes second order dynamical systems as well as fractional order dynamical systems. Have a watch! Please subscribe. And I look forward to a lively discussion. Music: Dream Away by Consolate Nobody Knows by Duckmaw Before the Dawn by Wild Beaches Clouds & Rainbows by Giants Nest Numb to It by Nbhd Nick Like a Blind Girls Dog by Daxten Overthinking by Dylan Sitts Guardians + Tek by Craig Hardgrove$

ThatMathThing |

Sampling theory and why I reject a lot of papers