@article{8773,
abstract = {Let g be a complex semisimple Lie algebra. We give a classification of contravariant forms on the nondegenerate Whittaker g-modules Y(χ,η) introduced by Kostant. We prove that the set of all contravariant forms on Y(χ,η) forms a vector space whose dimension is given by the cardinality of the Weyl group of g. We also describe a procedure for parabolically inducing contravariant forms. As a corollary, we deduce the existence of the Shapovalov form on a Verma module, and provide a formula for the dimension of the space of contravariant forms on the degenerate Whittaker modules M(χ,η) introduced by McDowell.},
author = {Brown, Adam and Romanov, Anna},
issn = {1088-6826},
journal = {Proceedings of the American Mathematical Society},
keywords = {Applied Mathematics, General Mathematics},
number = {1},
pages = {37--52},
publisher = {American Mathematical Society},
title = {{Contravariant forms on Whittaker modules}},
doi = {10.1090/proc/15205},
volume = {149},
year = {2021},
}
@article{6986,
abstract = {Li-Nadler proposed a conjecture about traces of Hecke categories, which implies the semistable part of the Betti geometric Langlands conjecture of Ben-Zvi-Nadler in genus 1. We prove a Weyl group analogue of this conjecture. Our theorem holds in the natural generality of reflection groups in Euclidean or hyperbolic space. As a corollary, we give an expression of the centralizer of a finite order element in a reflection group using homotopy theory. },
author = {Li, Penghui},
issn = {0002-9939},
journal = {Proceedings of the American Mathematical Society},
number = {11},
pages = {4597--4604},
publisher = {AMS},
title = {{A colimit of traces of reflection groups}},
doi = {10.1090/proc/14586},
volume = {147},
year = {2019},
}
@article{8495,
abstract = {In this note, we consider the dynamics associated to a perturbation of an integrable Hamiltonian system in action-angle coordinates in any number of degrees of freedom and we prove the following result of ``micro-diffusion'': under generic assumptions on $ h$ and $ f$, there exists an orbit of the system for which the drift of its action variables is at least of order $ \sqrt {\varepsilon }$, after a time of order $ \sqrt {\varepsilon }^{-1}$. The assumptions, which are essentially minimal, are that there exists a resonant point for $ h$ and that the corresponding averaged perturbation is non-constant. The conclusions, although very weak when compared to usual instability phenomena, are also essentially optimal within this setting.},
author = {Bounemoura, Abed and Kaloshin, Vadim},
issn = {0002-9939},
journal = {Proceedings of the American Mathematical Society},
number = {4},
pages = {1553--1560},
publisher = {American Mathematical Society},
title = {{A note on micro-instability for Hamiltonian systems close to integrable}},
doi = {10.1090/proc/12796},
volume = {144},
year = {2015},
}