Probability Seminar: Difference between revisions

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[[Probability | Back to Probability Group]]


= Fall 2020 =
* '''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


<b>Thursdays in 901 Van Vleck Hall at 2:30 PM</b>, unless otherwise noted.
[[Past Seminars]]
<b>We  usually end for questions at 3:20 PM.</b>


<b> IMPORTANT: </b> In Fall 2020 the seminar is being run online.
== Fall 2025 ==


If you would like to sign up for the email list to receive seminar announcements then please send an email to
<b>Thursdays at 2:30 PM either in 901 Van Vleck Hall or on Zoom</b>
[mailto:join-probsem@lists.wisc.edu join-probsem@lists.wisc.edu]


We usually end for questions at 3:20 PM.
== September 3, 2020, [https://math.wisc.edu TBA] (TBA) ==
'''TBA
'''


== September 4, 2025: No seminar ==


== September 10, 2020, ==
== 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.


== October 1, 2020, [https://marcusmichelen.org/ Marcus Michelen], [https://mscs.uic.edu/ UIC] ==
== September 18, 2025: Je Paguyo (McMaster U.) ==


Title: '''TBA'''
== September 25, 2025: Chris Janjigian (Purdue U.) ==


Abstract: TBA
== October 2, 2025: Elliot Paquette (McGill U.) ==


== October 9, 2025: No seminar (Midwest Probability Colloquium) ==


[[Past Seminars]]
== 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

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

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.


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)