Probability Seminar: Difference between revisions
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[[Probability | Back to Probability Group]] | |||
* '''When''': Thursdays at 2:30 pm | |||
* '''Where''': 901 Van Vleck Hall | |||
* '''Organizers''': Hongchang Ji, Ander Aguirre, Hai-Xiao Wang | |||
* '''To join the probability seminar mailing list:''' email probsem+subscribe@g-groups.wisc.edu. | |||
* '''To subscribe seminar lunch announcements:''' email lunchwithprobsemspeaker+subscribe@g-groups.wisc.edu | |||
[[Past Seminars]] | |||
== Fall 2025 == | |||
<b>Thursdays at 2:30 PM either in 901 Van Vleck Hall or on Zoom</b> | |||
We usually end for questions at 3:20 PM. | |||
== September 4, 2025: No seminar == | |||
== September | == September 11, 2025: David Renfrew (Binghamton U.) == | ||
'''Singularities in the spectrum of random block matrices''' | |||
We consider the density of states of structured Hermitian and non-Hermitian random matrices with a variance profile. As the dimension tends to infinity the associated eigenvalue density can develop a singularity at the origin. The severity of this singularity depends on the relative positions of the zero submatrices. We provide a classification of all possible singularities and determine the exponent in the density blow-up. | |||
== | == September 18, 2025: Je Paguyo (McMaster U.) == | ||
== September 25, 2025: Chris Janjigian (Purdue U.) == | |||
== October 2, 2025: Elliot Paquette (McGill U.) == | |||
== October 9, 2025: No seminar (Midwest Probability Colloquium) == | |||
== October 16, 2025: Zachary Selk (Florida State U.) == | |||
'''<br />On the Onsager-Machlup Function for the \Phi^4 Measure''' | |||
The \Phi^4 measure is a measure arising in effective quantum field theory as arguably the simplest example of a nontrivial QFT, modelling the self-interaction of a single scalar quantum field. This measure can be constructed through a procedure known as stochastic quantization. Stochastic quantization seeks to construct a measure on an infinite dimensional space with a given Gibbs-type ``density function" as the invariant measure of a stochastic PDE, in analogy with Langevin dynamics of stochastic ODEs. Both the \Phi^4 measure and its associated stochastic quantization PDE involve nonlinearities of distributions, necessitating renormalization procedures via tools like Wick calculus, regularity structures or paracontrolled calculus. Although the \Phi^4 measure has been constructed in dimensions 1,2 and 3, the question of whether these measures have the desired ``density function" remains open. Although in infinite dimensions, density functions are typically thought to not exist as there is no reference Lebesgue measure, there is a notion of a probability density function that extends to infinite dimensions called the Onsager-Machlup (OM) functional. One pathology of OM theory is that different metrics can lead to different OM functionals, or OM functionals can fail to exist under reasonable metrics. In a joint work with Ioannis Gasteratos (TU Berlin), we study the OM functional for the \Phi^4 measure. In dimension 1, the OM functional is what is desired under naive choices of metrics. In dimension 2, the OM functional is what is desired if we choose a metric analogous to the rough paths metric. In dimension 3, naive approaches don't work and the situation is complicated. | |||
==October 23, 2025: Alex Dunlap (Duke U.)== | |||
==October 30, 2025: Ander Aguirre (UW-Madison)== | |||
==November 6, 2025: Sudeshna Bhattacharjee (Indian Institute of Science)== | |||
== November 13, 2025: Jiaoyang Huang (U. Penn) == |
Latest revision as of 22:44, 27 August 2025
- When: Thursdays at 2:30 pm
- Where: 901 Van Vleck Hall
- Organizers: Hongchang Ji, Ander Aguirre, Hai-Xiao Wang
- To join the probability seminar mailing list: email probsem+subscribe@g-groups.wisc.edu.
- To subscribe seminar lunch announcements: email lunchwithprobsemspeaker+subscribe@g-groups.wisc.edu
Fall 2025
Thursdays at 2:30 PM either in 901 Van Vleck Hall or on Zoom
We usually end for questions at 3:20 PM.
September 4, 2025: No seminar
September 11, 2025: David Renfrew (Binghamton U.)
Singularities in the spectrum of random block matrices
We consider the density of states of structured Hermitian and non-Hermitian random matrices with a variance profile. As the dimension tends to infinity the associated eigenvalue density can develop a singularity at the origin. The severity of this singularity depends on the relative positions of the zero submatrices. We provide a classification of all possible singularities and determine the exponent in the density blow-up.
September 18, 2025: Je Paguyo (McMaster U.)
September 25, 2025: Chris Janjigian (Purdue U.)
October 2, 2025: Elliot Paquette (McGill U.)
October 9, 2025: No seminar (Midwest Probability Colloquium)
October 16, 2025: Zachary Selk (Florida State U.)
On the Onsager-Machlup Function for the \Phi^4 Measure
The \Phi^4 measure is a measure arising in effective quantum field theory as arguably the simplest example of a nontrivial QFT, modelling the self-interaction of a single scalar quantum field. This measure can be constructed through a procedure known as stochastic quantization. Stochastic quantization seeks to construct a measure on an infinite dimensional space with a given Gibbs-type ``density function" as the invariant measure of a stochastic PDE, in analogy with Langevin dynamics of stochastic ODEs. Both the \Phi^4 measure and its associated stochastic quantization PDE involve nonlinearities of distributions, necessitating renormalization procedures via tools like Wick calculus, regularity structures or paracontrolled calculus. Although the \Phi^4 measure has been constructed in dimensions 1,2 and 3, the question of whether these measures have the desired ``density function" remains open. Although in infinite dimensions, density functions are typically thought to not exist as there is no reference Lebesgue measure, there is a notion of a probability density function that extends to infinite dimensions called the Onsager-Machlup (OM) functional. One pathology of OM theory is that different metrics can lead to different OM functionals, or OM functionals can fail to exist under reasonable metrics. In a joint work with Ioannis Gasteratos (TU Berlin), we study the OM functional for the \Phi^4 measure. In dimension 1, the OM functional is what is desired under naive choices of metrics. In dimension 2, the OM functional is what is desired if we choose a metric analogous to the rough paths metric. In dimension 3, naive approaches don't work and the situation is complicated.