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Contents
0
Introduction
1
Electromagnetic duality and monopoles
1.1
Electric and magnetic charges
1.2
The S and the T transformations
1.3
’t Hooft-Polyakov monopoles
1.3.1
Classical features
1.3.2
Semiclassical features
2
𝒩
=
2
multiplets and Lagrangians
2.1
Microscopic Lagrangian
2.1.1
𝒩
=
1
superfields
2.1.2
Vector multiplets and hypermultiplets
2.2
Vacua
2.3
BPS bound
2.4
Low energy Lagrangian
3
Renormalization and anomaly
3.1
Renormalization
3.2
Anomalies
3.2.1
Anomalies of global symmetry
3.2.2
Anomalies of gauge symmetry
3.3
𝒩
=
1
pure Yang-Mills
3.3.1
Confinement and gaugino condensate
3.3.2
The theory in a box
4
Seiberg-Witten solution to pure
S
U
(
2
)
theory
4.1
One-loop running and the monodromy at infinity
4.2
Behavior in the strongly-coupled region
4.3
The Seiberg-Witten solution
4.3.1
The curve
4.3.2
The monodromy
M
∞
4.3.3
The monodromies
M
±
4.4
Less supersymmetric cases
4.4.1
𝒩
=
1
system
4.4.2
Pure bosonic system
4.5
S
U
(
2
)
vs
S
O
(
3
)
5
S
U
(
2
)
theory with one flavor
5.1
Structure of the
u
-plane
5.1.1
Schematic running of the coupling
5.1.2
Monodromies
5.2
The curve
5.3
Some notable features
6
Curves and 6d
𝒩
=
(
2
,
0
)
theory
6.1
Strings with variable tension
6.2
Strings with variable tension from membranes
6.2.1
General idea
6.2.2
Example: pure
S
U
(
2
)
theory
6.3
Self-duality of the 6d theory
6.4
Intermediate 5d Yang-Mills theory and its boundary conditions
6.4.1
Five-dimensional maximally-supersymmetric Yang-Mills
6.4.2
𝒩
=
4
super Yang-Mills
6.4.3
𝒩
=
2
pure
S
U
(
2
)
theory and the
N
f
=
1
theory
6.4.4
The
S
U
(
2
)
theories with
N
f
=
2
,
3
,
4
7
Higgs branches and hyperkähler manifolds
7.1
General structures of the Higgs branch Lagrangian
7.2
Hypermultiplets revisited
7.3
The hyperkähler quotient
7.3.1
U
(
1
)
gauge theory with one charged hypermultiplet
7.3.2
S
U
(
2
)
gauge theory with two hypermultiplets in the doublet
8
S
U
(
2
)
theory with 2 and 3 flavors
8.1
Generalities
8.2
N
f
=
2
: the curve and the monodromies
8.3
N
f
=
2
: the discrete R-symmetry
8.4
N
f
=
2
: the moduli space
8.5
N
f
=
3
9
S
U
(
2
)
theory with 4 flavors and Gaiotto’s duality
9.1
The curve as
λ
2
=
ϕ
2
(
z
)
9.2
Identification of parameters
9.2.1
Coupling constant
9.2.2
Mass parameters
9.3
Weak-coupling limit and trifundamentals
9.4
Strong-coupling limit
9.5
Generalization
9.5.1
Trivalent diagrams
9.5.2
Example: torus with one puncture
9.5.3
Example: sphere with five punctures
9.5.4
Example: a genus-two surface
9.5.5
The curve and the Hitchin field
9.6
Theories with less flavors revisited
9.6.1
Rewriting of the curves
9.6.2
Generalization
10
Argyres-Douglas CFTs
10.1
N
f
=
1
theory and the simplest Argyres-Douglas CFT
10.2
Argyres-Douglas CFT from the
N
f
=
2
theory
10.3
Argyres-Douglas CFT from the
N
f
=
3
theory
10.4
Summary of rank-1 theories
10.4.1
Argyres-Douglas CFTs from
S
U
(
2
)
with flavors
10.4.2
Exceptional theories of Minahan-Nemeschansky
10.4.3
Newer rank-1 theories
10.5
More general Argyres-Douglas CFTs:
X
N
and
Y
N
11
Theories with other simple gauge groups
11.1
Semiclassical analysis
11.2
Pure
S
U
(
N
)
theory
11.2.1
The curve
11.2.2
Infrared gauge coupling matrix
11.3
S
U
(
N
)
theory with fundamental flavors
11.3.1
N
f
=
1
11.3.2
General number of flavors
11.4
S
O
(
2
N
)
theories
11.4.1
Semi-classical analysis
11.4.2
Pure
S
O
(
2
N
)
theory
11.4.3
S
O
(
2
N
)
theory with flavors in the vector representation
11.5
Argyres-Douglas CFTs
11.5.1
Pure
S
U
(
N
)
theory
11.5.2
S
U
(
N
)
theory with two flavors
11.5.3
Pure
S
O
(
2
N
)
theory
11.5.4
Argyres-Douglas CFTs and the Higgs branch
11.6
Seiberg-Witten solutions for various other simple gauge groups
12
Argyres-Seiberg-Gaiotto duality for
S
U
(
N
)
theory
12.1
S-dual of
S
U
(
N
)
with
N
f
=
2
N
flavors, part I
12.1.1
Rewriting of the curve
12.1.2
Weak-coupling limit
12.1.3
A strong-coupling limit
12.2
S
U
(
N
)
quiver theories and tame punctures
12.2.1
Quiver gauge theories
12.2.2
𝒩
=
2
∗
theory
12.2.3
Linear quiver theories
12.2.4
Tame punctures
12.2.5
Tame punctures and the number of Coulomb branch operators
12.2.6
Tame punctures and the decoupling
12.3
S-dual of
S
U
(
N
)
with
N
f
=
2
N
flavors, part II
12.3.1
For general
N
12.3.2
N
=
3
: Argyres-Seiberg duality
12.4
Applications
12.4.1
T
N
12.4.2
M
N
(
E
7
)
12.4.3
M
N
(
E
8
)
12.4.4
The singular limit of
S
U
(
N
)
with even number of flavors
12.5
Tame punctures and Higgsing
13
Conclusions and further directions
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