On quantitative chaos of rescaled states
- Series
- Math Physics Seminar
- Time
- Friday, November 14, 2025 - 11:00 for 1 hour (actually 50 minutes)
- Location
- Zoom and streamed in Skiles 006
- Speaker
- Hagop Tossounian – Universidad de Concepción
Please Note: In order to derive his equation, Boltzmann used the assumption that the probability density function f(t,x1,v1, x2,v2, ..., xN,vN), describing the positions and velocities of a gas of N identical particles at time t, stays close to a product g(t,x1,v1) g(t,x2,v2)...g(t,xN,vN). Here g is the common 1-particle distribution. Mark Kac introduced a probabilistic model for N particles, for which Boltzmann's assumption is valid as N goes to infinity in a specific sense, provided that it is valid at an initial time. Kac's requirement concerning the N particle density functions at some initial time is nowadays known as chaos (or molecular chaos), and Kac's result is known as propagation of chaos. The aim of this talk is to retake the question, first asked and studied in [CCLLV] : For which density functionals g can we produce a family of symmetric densities {fN} supported on the constant energy sphere {v1^2+v2^2+ ... + vN^2 = N} which are chaotic to g? Using rescaled states, we show [CT] that the class of admissible g, obtained in [CCLLV] using other methods, can be expanded. We also mention some new ideas in this direction. This talk is introductory. References: [CCLLV] Carlen, Eric A., et al. "Entropy and chaos in the Kac model." Kinetic and Related Models 3.1 (2010): 85-122. [CT] Cortez, Roberto, and Hagop Tossounian. "Chaos for rescaled measures on Kac’s sphere." Electronic Journal of Probability 28 (2023): 1-29.