Other teams n Kumar, Park, Taylor n Grimm, Hayashi n Krause, Mayrhofer, Weigand n Hayashi, Lawrie, Morisson , Schafer-Nameki... Other teams n Kumar, Park, Taylor n Grimm, H
Trang 2Other teams
n Kumar, Park, Taylor
n Grimm, Hayashi
n Krause, Mayrhofer, Weigand
n Hayashi, Lawrie, Morisson , Schafer-Nameki
Trang 3Other teams
n Kumar, Park, Taylor
n Grimm, Hayashi
n Krause, Mayrhofer, Weigand
n Hayashi, Lawrie, Morisson , Schafer-Nameki
Love to my other collaborators:
Paolo Aluffi
Patrick Jefferson
Michele Del Zotto, Jonathan Heckman, Cumrun Vafa
Trang 4It also comes as a combo:
…an elliptic fibration
Trang 5+ Tale of two worlds
Gauge theories Elliptic fibrations
Gauge algebra Codimension one singularities Representations Codimension two singularities
Coulomb phases Crepant resolutions
Phase transitions Flops
Trang 75D supersymmetric gauge theories with
8 supercharges
Geometry:
Trang 8Coulomb branch of 5D gauge theory
n Vector multiplets-> Weyl chamber
n Massless Hypers at singularities -> sub-chamber structure
Trang 9Incidence geometry of a representation R
n g is a Lie algebra with Cartan sub-algebra h
n Roots of g define Weyl chambers
n R : a representation of g
n Weights of R refine the Weyl chambers by adding a chamber structure
Trang 12n Miranda models (collisions of singularities)
n Szydlo (generalization of Miranda’s model and Tate’s algorithm)
Trang 131 3
2
In?
i i
@
@ i i i i
@
i i
Trang 20The case of SU(3)
1 1
1 1
I ∗ 0
1 1
Trang 28Tree of resolutions for SU(4)
1 1
1 1
I5
1
1 1
1
1 1
1 1
1 1
Trang 29A perfect match!
Trang 33+