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directed polymers
The Green's function of the parabolic Anderson model and the continuum directed polymer
Tom Alberts
,
Chris Janjigian
,
Firas Rassoul-Agha
,
Timo Seppalainen
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Busemann functions and semi-infinite O'Connell-Yor polymers
We prove that given any fixed asymptotic velocity, the finite length O’Connell-Yor polymer has an infinite length limit …
Tom Alberts
,
Firas Rassoul-Agha
,
Mackenzie Simper
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DOI
Macro and Microscopic Limits of Directed Polymer Models
Busemann functions for the O’Connell-Yor polymer
Jun 4, 2019 16:30 +0800 — 17:30 +0800
KAIST
Tom Alberts
,
Firas Rassoul-Agha
,
Mackenzie Simper
Macro and Microscopic Limits of Directed Polymer Models
Busemann functions for the O’Connell-Yor polymer
May 31, 2019 16:00 +0800 — 17:30 +0800
Korean Institute of Advanced Study
Tom Alberts
,
Firas Rassoul-Agha
,
Mackenzie Simper
Nested critical points for a directed polymer on a disordered diamond lattice
We consider a model for a directed polymer in a random environment defined on a hierarchical diamond lattice in which i.i.d. random …
Tom Alberts
,
Jeremy Clark
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The intermediate disorder regime for a directed polymer model on a hierarchical lattice
We study a directed polymer model defined on a hierarchical diamond lattice, where the lattice is constructed recursively through a …
Tom Alberts
,
Jeremy Clark
,
Saša Kocić
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DOI
Airy Processes and Variational Formulas, Part II
Review of the Quastel-Remenik work on Airy processes and variational formulas
Sep 16, 2016 15:00 -0700 — 16:00 -0700
University of Utah
Tom Alberts
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Airy Processes and Variational Formulas, Part I
Review of the Quastel-Remenik work on Airy processes and variational formulas
Sep 9, 2016 15:00 -0700 — 16:00 -0700
University of Utah
Tom Alberts
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Slides
Ideas from KPZ in Directed Polymer Models
KPZ scalings in directed polymer models
Apr 17, 2016 09:00 MDT — 09:30 MDT
North Dakota State University
Tom Alberts
The intermediate disorder regime for directed polymers in dimension $1+1$
We introduce a new disorder regime for directed polymers in dimension $1+1$ that sits between the weak and strong disorder regimes. We …
Tom Alberts
,
Konstantin Khanin
,
Jeremy Quastel
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