Javascript must be enabled to continue!
Noncommutative resolutions and CICY quotients from a non-Abelian GLSM
View through CrossRef
We discuss a one-parameter non-Abelian GLSM with gauge group
(U(1)× U(1)× U(1))\rtimes\mathbb{Z}_3
(
U
(
1
)
×
U
(
1
)
×
U
(
1
)
)
⋊
ℤ
3
and its associated Calabi-Yau phases. The large volume phase is a free
\mathbb{Z}_3
ℤ
3
-quotient of a codimension
3
3
complete intersection of degree-
(1,1,1)
(
1
,
1
,
1
)
hypersurfaces in
\mathbb{P}^2×\mathbb{P}^2×\mathbb{P}^2
ℙ
2
×
ℙ
2
×
ℙ
2
. The associated Calabi-Yau differential operator has a second point of maximal unipotent monodromy, leading to the expectation that the other GLSM phase is geometric as well. However, the associated GLSM phase appears to be a hybrid model with continuous unbroken gauge symmetry and cubic superpotential, together with a Coulomb branch. Using techniques from topological string theory and mirror symmetry we collect evidence that the phase should correspond to a non-commutative resolution, in the sense of Katz-Klemm-Schimannek-Sharpe, of a codimension two complete intersection in weighted projective space with
63
63
nodal points, for which a resolution has
\mathbb{Z}_3
ℤ
3
-torsion. We compute the associated Gopakumar-Vafa invariants up to genus
11
11
, incorporating their torsion refinement. We identify two integral symplectic bases constructed from topological data of the mirror geometries in either phase.
Title: Noncommutative resolutions and CICY quotients from a non-Abelian GLSM
Description:
We discuss a one-parameter non-Abelian GLSM with gauge group
(U(1)× U(1)× U(1))\rtimes\mathbb{Z}_3
(
U
(
1
)
×
U
(
1
)
×
U
(
1
)
)
⋊
ℤ
3
and its associated Calabi-Yau phases.
The large volume phase is a free
\mathbb{Z}_3
ℤ
3
-quotient of a codimension
3
3
complete intersection of degree-
(1,1,1)
(
1
,
1
,
1
)
hypersurfaces in
\mathbb{P}^2×\mathbb{P}^2×\mathbb{P}^2
ℙ
2
×
ℙ
2
×
ℙ
2
.
The associated Calabi-Yau differential operator has a second point of maximal unipotent monodromy, leading to the expectation that the other GLSM phase is geometric as well.
However, the associated GLSM phase appears to be a hybrid model with continuous unbroken gauge symmetry and cubic superpotential, together with a Coulomb branch.
Using techniques from topological string theory and mirror symmetry we collect evidence that the phase should correspond to a non-commutative resolution, in the sense of Katz-Klemm-Schimannek-Sharpe, of a codimension two complete intersection in weighted projective space with
63
63
nodal points, for which a resolution has
\mathbb{Z}_3
ℤ
3
-torsion.
We compute the associated Gopakumar-Vafa invariants up to genus
11
11
, incorporating their torsion refinement.
We identify two integral symplectic bases constructed from topological data of the mirror geometries in either phase.
Related Results
GLSM realizations of maps and intersections of Grassmannians and Pfaffians
GLSM realizations of maps and intersections of Grassmannians and Pfaffians
Abstract
In this paper we give gauged linear sigma model (GLSM) realizations of a number of geometries not previously presented in GLSMs. We begin by describin...
UN Resolutions as 'Hard-Law' in Armed Conflict
UN Resolutions as 'Hard-Law' in Armed Conflict
The sources of international law, as codified in Article 38 of the Statute of the International Court of Justice (ICJ) – international conventions; international custom; the genera...
Noncommutative Solutions to Zamolodchikov's Tetrahedron Equation and Matrix Six-Factorisation Problems
Noncommutative Solutions to Zamolodchikov's Tetrahedron Equation and Matrix Six-Factorisation Problems
It is known that the local Yang–Baxter equation is a generator of potential solutions to Zamolodchikov’s tetrahedron equation. In this paper, we show under which additional conditi...
The Removal Lemma: algebraic versions and applications
The Removal Lemma: algebraic versions and applications
This thesis presents some contributions in additive combinatorics and arithmetic Ramsey theory. More specifically, it deals with the interaction between combinatorics, number theor...
Characterizing asymptotic randomization in abelian cellular automata
Characterizing asymptotic randomization in abelian cellular automata
Abelian cellular automata (CAs) are CAs which are group endomorphisms of the full group shift when endowing the alphabet with an abelian group structure. A CA randomizes an initial...
Gauge Theories in Rainbow Space-Time
Gauge Theories in Rainbow Space-Time
We construct Maxwell and Yang-Mills theories in the rainbow space-time. We show that the time-dependent Aharonov-Bohm phases for both Abelian and non-Abelian gauge fields are non-z...
A Poincaré covariant noncommutative spacetime
A Poincaré covariant noncommutative spacetime
We interpret, in the realm of relativistic quantum field theory, the tangential operator given by Coleman and Mandula [All possible symmetries of the [Formula: see text] matrix, Ph...
Derived equivalence and homological projective duality in GLSM
Derived equivalence and homological projective duality in GLSM
Brane transport provides a way to realize functors between the categories of B-branes of different phases in gauged linear sigma model (GLSM). When appropriately designed, these fu...

