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Singularities and in the University

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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

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Other teams

n   Kumar, Park, Taylor

n   Grimm, Hayashi

n   Krause, Mayrhofer, Weigand

n   Hayashi, Lawrie, Morisson , Schafer-Nameki

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Other 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

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It also comes as a combo:

…an elliptic fibration

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+ Tale of two worlds

Gauge theories Elliptic fibrations

Gauge algebra Codimension one singularities Representations Codimension two singularities

Coulomb phases Crepant resolutions

Phase transitions Flops

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5D supersymmetric gauge theories with

8 supercharges

Geometry:

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Coulomb branch of 5D gauge theory

n   Vector multiplets-> Weyl chamber

n   Massless Hypers at singularities -> sub-chamber structure

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Incidence 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

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n   Miranda models (collisions of singularities)

n   Szydlo (generalization of Miranda’s model and Tate’s algorithm)

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1 3

2

In?

i i

@

@ i i i i

@

i i

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The case of SU(3)

1 1

1 1

I ∗ 0

1 1

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Tree of resolutions for SU(4)

1 1

1 1

I5

1

1 1

1

1 1

1 1

1 1

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A perfect match!

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