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AGT関係式とその一般化に向けて
(String Advanced Lectures No.22)
高エネルギー加速器研究機構(KEK)
素粒子原子核研究所(IPNS)
柴 正太郎
2010年7月5日(月) 14:00-15:40
Contents
1. Gaiotto‟s discussion
2. AGT relation for SU(2) quiver theories
3. AGT-W relation for SU(N) quiver theories
4. AdS/CFT correspondence of AGT‟s system
Gaiotto‟s discussion
Seiberg-Witten curve
Low energy effective action (by Wilson‟s renormalization : integration out of massive fields)
prepotential
potential for scalar field
4-dim N=2 SU(2) supersymmetric gauge theory [Seiberg-Witten ‟94]
classical 1-loop instanton
: energy scale
: Higgs potential (which breaks gauge symmetry)
This breakdown is parametrized by
u (VEV) : shift of color brane
mass : shift of flavor brane
Singular points of prepotential, Seiberg-Witten curve and S-duality
The singular points of prepotential on u-plane
By studying the monodromy of and , we can find that the
prepotential has singular points. This can be described as
• These singular points means the emergence of new massless fields.
• This means that the prepotential must become a different form near a different
singular point. ( S-duality)
M-theory interpretation : singular points are intersection points of M5-branes.
(or D4/NS5-branes)
[Witten ‟97]
: Seiberg-Witten curve in
coupling
SU(2) generalized quivers[Gaiotto ‟09]
SU(2) gauge theory with 4 fundamental flavors (hypermultiplets)
S-duality group SL(2,Z)
coupling const. :
flavor sym. : SO(8) ⊃ SO(4)×SO(4) ~ [SU(2)a×SU(2)b]×[SU(2)c×SU(2)d]
: (elementary) quark
: monopole
: dyon
D4
NS5
Subgroup of S-duality without permutation of masses
In massive case, we especially consider this subgroup.
• mass : mass parameters can be associated to each SU(2) flavor.
Then the mass eigenvalues of four hypermultiplets in 8v is , .
• coupling : cross ratio (moduli) of the four punctures, i.e. z=
Actually, this is equal to the exponential of the UV coupling
→ This is an aspect of correspondence between the 4-dim N=2 SU(2) gauge
theory and the 2-dim Riemann surface with punctures.
SU(2) gauge theory with massive fundamental hypermultiplets
SU(2)1×SU(2)2 gauge theory with fundamental and bifundamental flavors
• When each gauge group is coupled to 4 flavors, this theory is conformal.
• flavor symmetry ⊃ [SU(2)a×SU(2)b]×SU(2)e×[SU(2)c×SU(2)d]
flavor sym. of bifundamental hyper. : Sp(1) ~ SU(2) i.e. real representation
• S-duality subgroup without permutation of masses
When the gauge coupling of SU(2)2 vanishes or is very weak, we can discuss it
in the same way as before for SU(2)1. The similar discussion goes for (1 2).
That is, this subgroup consists of the permutation of five SU(2)‟s.
cf. Note that two SL(2,Z) full S-duality groups do not commute! Here, we
analyze only the boundary of the gauge coupling moduli space.
SU(2)1×SU(2)2×SU(2)3 gauge theory with fund. and bifund. flavors
(The similar discussion goes.)
■, ■ : weak: interchange
turn on/off a gauge coupling
For more generalized SU(2) quivers : more gauge groups, loops…
Seiberg-Witten curve for quiver SU(2) gauge theories
massless SU(2) case
In this case, the Seiberg-Witten curve is of the form
If we change the variable as , this becomes
massless SU(2) n case
or
mass deformation
The number of mass parameters is n+3, because of the freedom .
where are
the solutions ofVEV coupling
polynomial of z of (n-1)-th order
divergent at punctures
SU(3) generalized quivers
SU(3) gauge theory with 6 fundamental flavors (hypermultiplets)
• This theory is also conformal.
• flavor symmetry U(6) : complex rep. of SU(3) gauge group
• kind of S-duality group : Argyres-Seiberg duality [Argyres-Seiberg ‟07]
coupling const. :
flavor : U(6) ⊃ [SU(3)×U(1)]×[SU(3)×U(1)] : weak coupling
U(6) ⊃ SU(6)×U(1) ~ [SU(3)×SU(3)×U(1)]×U(1)
SU(6)×SU(2) ⊂ E6 : infinite coupling of SU(3) theory
Moreover, weakly coupled gauge group becomes SU(2) instead of SU(3) !
breakdown by VEV
Argyres-Seiberg duality for SU(3) gauge theory
infinite coupling
D4
NS5
SU(3)1×SU(3)2 gauge theory with fundamental and bifundamental flavors
flavor symmetry of bifundamental
Argyres-Seiberg duality
For more generalized SU(3) quivers : more gauge groups, loops…
turn on/off a gauge coupling
Seiberg-Witten curve for SU(3) quiver gauge theories
massless SU(3)n case
massless SU(2)×SU(3)n-2×SU(2) case
mass deformation
massless :
massive :
The number of mass parameters is n+3, because of the freedom .
In both cases, SW curve can be rewritten as ( ),
but the order of divergence of is different from each other.
SU(N) generalized quivers
Seiberg-Witten curve in this case is of the form
The variety of quiver gauge group
where
is reflected in the various order of divergence of at punctures.
For example…
Seiberg-Witten curve for massless SU(N) quiver gauge theories
SU(2) quiver case
• order of divergence :
• mass parameters :
• flavor symmetry : SU(2)
SU(3) quiver case
• order of divergence :
• mass parameters :
• flavor symmetry : U(1) SU(3)
Classification of punctures : divergence of massless SW curve at punctures
SU(3) quiver case
corresponding puncture :
SU(4) quiver case (and the natural analogy is valid for general SU(N) case)
Classification of punctures : divergence of massless SW curve at punctures
AGT relation for SU(2) quivers
SU(2) partition function
We now consider only the linear quiver gauge theories in AGT relation.
Gaiotto‟s discussion
Nekrasov‟s partition function of 4-dim gauge theory
Action
classical part
1-loop correction : more than 1-loop is cancelled, because of N=2 SUSY.
instanton correction : Nekrasov‟s calculation with Young tableaux
Parameters
coupling constants
masses of fundamental / antifund. / bifund. fields and VEV‟s of gauge fields
deformation parameters :
background of graviphoton or deformation (rotation) of extra dimensions
(Note that they are different from Gaiotto‟s ones!)
Now we calculate Nekrasov‟s partition function of 4-dim SU(2) quiver gauge
theory as the quantity of interest.
D4
NS5
1-loop part of partition function of 4-dim quiver gauge theory
We can obtain it of the analytic form :
where each factor is defined as
: each factor is a product of double Gamma function!
,
gauge antifund. bifund. fund.
mass massmassVEV
deformation parameters
We obtain it of the expansion form of instanton number :
where : coupling const. and
and
Instanton part of partition function of 4-dim quiver gauge theory
Young tableau
< Young tableau >
instanton # = # of boxes
leg
arm
The Nekrasov partition function for the simple case of SU(2) with four flavors is
Since the mass dimension of is 1, so we fix the scale as , .(by definition)
Mass parameters : mass eigenvalues of four hypermultiplets
• : mass parameters of
• : mass parameters of
VEV‟s : we set --- decoupling of U(1) (i.e. trace) part.
We must also eliminate the contribution from U(1) gauge multiplet.
This makes the flavor symmetry SU(2)i×U(1)i enhanced to SU(2)i×SU(2)i.(next page…)
SU(2) with four flavors : Calculation of Nekrasov function for U(2)
U(2), actually
Manifest flavor symmetry is now
U(2)0×U(2)1 , while actual symmetry is
SO(8)⊃[SU(2)×SU(2)]×[SU(2)×SU(2)].
In this case, Nekrasov partition function can be written as
where and
is invariant under the flip (complex conjugate representation) :
which can be regarded as the action of Weyl group of SU(2) gauge symmetry.
is not invariant. This part can be regarded as U(1) contribution.
Surprising discovery by Alday-Gaiotto-Tachikawa
In fact, is nothing but the conformal block of Virasoro algebra with
for four operators of dimensions inserted at :
SU(2) with four flavors : Identification of SU(2) part and U(1) part
(intermediate state)
Correlation function of Liouville theory with .
Thus, we naturally choose the primary vertex operator as the
examples of such operators. Then the 4-point function on a sphere is
3-point function conformal block
where
The point is that we can make it of the form of square of absolute value!
… only if
… using the properties : and
Liouville correlation function
As a result, the 4-point correlation function can be rewritten as
where and
It says that the 3-point function (DOZZ factor) part also can be written as
the product of 1-loop part of 4-dim SU(2) partition function :
under the natural identification of mass parameters :
Example 1 : SU(2) with four flavors (Sphere with four punctures)
Example 2 : Torus with one puncture
The SW curve in this case corresponds to 4-dim N=2* theory :
N=4 SU(2) theory deformed by a mass for the adjoint hypermultiplet
Nekrasov instanton partition function
This can be written as
where equals to the conformal block of Virasoro algebra with
Liouville correlation function (corresponding 1-point function)
where is Nekrasov‟s partition function.
Example 3 : Sphere with multiple punctures
The Seiberg-Witten curve in this case corresponds to
4-dim N=2 linear quiver SU(2) gauge theory.
Nekrasov instanton partition function
where equals to the conformal block of
Virasoro algebra with for the vertex operators which are inserted
at z=
Liouville correlation function (corresponding n+3-point function)
where is Nekrasov‟s full partition function.
(↑ including 1-loop part)
U(1) part
[Alday-Gaiotto-Tachikawa ‟09]AGT relation : SU(2) gauge theory Liouville theory !
Gauge theory Liouville theory
coupling const. position of punctures
VEV of gauge fields internal momenta
mass of matter fields external momenta
1-loop part DOZZ factors
instanton part conformal blocks
deformation parameters Liouville parameters
4-dim theory : SU(2) quiver gauge theory
2-dim theory : Liouville (A1 Toda) field theory
In this case, the 4-dim theory‟s partition function Z and the 2-dim theory‟s
correlation function correspond to each other :
central charge :
• According to Gaiotto‟s discussion, SW curve for SU(2) case is .
• In massive cases, has double poles.
• Then the mass parameters can be obtained as ,
where is a small circle around the a-th puncture.
• The other moduli can be fixed by the special coordinates ,
where is the i-th cycle (i.e. long tube at weak coupling).
Note that the number of these moduli is 3g-3+n.
(g : # of genus, n : # of punctures)
SW curve and AGT relation
Seiberg-Witten curve and its moduli
• The Seiberg-Witten curve is supposed to emerge from Nekrasov partition
function in the “semiclassical limit” , so in this limit, we expect
that .
• In fact, is satisfied on a sphere,
then has double poles at zi .
• For mass parameters, we have ,
where we use and .
• For special coordinate moduli, we have ,
which can be checked by order by order calculation in concrete examples.
• Therefore, it is natural to speculate that Seiberg-Witten curve is „quantized‟
to at finite .
2-dim CFT in AGT relation : „quantization‟ of Seiberg-Witten curve??
AGT-W relation for SU(N)
Now we calculate Nekrasov‟s partition function of 4-dim SU(N) quiver gauge
theory as the quantity of interest.
SU(2) case : We consider only SU(2)×…×SU(2) quiver gauge theories.
SU(N) case : According to Gaiotto‟s discussion, we consider, in general, the
cases of SU(d1) x SU(d2) x … x SU(N) x … x SU(N) x … x SU(d‟2) x SU(d‟1) group,
where is non-negative.
SU(N) partition function
Nekrasov‟s partition function of 4-dim gauge theory
xx xx
x
*
…x
*
…
…
d‟3–d‟2d‟2–d‟1d‟1… …
……
…
d3–d2
d2–d1
d1… ………
1-loop part of partition function of 4-dim quiver gauge theory
We can obtain it of the analytic form :
where each factor is defined as
: each factor is a product of double Gamma function!
,
gauge antifund. bifund. fund.
mass massmass
flavor symm. of bifund. is U(1)
VEV
# of d.o.f. depends on dk
deformation parameters
We obtain it of the expansion form of instanton number :
where : coupling const. and
and
Instanton part of partition function of 4-dim quiver gauge theory
Young tableau
< Young tableau >
instanton # = # of boxes
leg
arm
Naive assumption is 2-dim AN-1 Toda theory, since Liouville theory is nothing but
A1 Toda theory. This means that the generalized AGT relation seems
Difference from SU(2) case…
• VEV‟s in 4-dim theory and momenta in 2-dim theory have more than one d.o.f.
In fact, the latter corresponds to the fact that the punctures are classified with
more than one kinds of N-box Young tableaux :
< full-type > < simple-type > < other types >
(cf. In SU(2) case, all these Young tableaux become ones of the same type .)
• In general, we don‟t know how to calculate the conformal blocks of Toda theory.
……
…
…
………
What kind of 2-dim CFT corresponds to 4-dim SU(N) quiver gauge theory?
Action :
Toda field with :
It parametrizes the Cartan subspace of AN-1 algebra.
simple root of AN-1 algebra :
Weyl vector of AN-1 algebra :
metric and Ricci scalar of 2-dim surface
interaction parameters : b (real) and
central charge :
Toda theory and W-algebra
What is AN-1 Toda theory? : some extension of Liouville theory
• In this theory, there are energy-momentum tensor and higher spin fields
as Noether currents.
• The symmetry algebra of this theory is called W-algebra.
• For the simplest example, in the case of N=3, the generators are defined as
And, their commutation relation is as follows:
which can be regarded as the extension of Virasoro algebra, and where
,
What is AN-1 Toda field theory? (continued)
We ignore Toda potential
(interaction) at this stage.
• The primary fields are defined as ( is called „momentum‟) .
• The descendant fields are composed by acting / on the primary
fields as uppering / lowering operators.
• First, we define the highest weight state as usual :
Then we act lowering operators on this state, and obtain various descendant
fields as .
• However, some linear combinations of descendant fields accidentally satisfy
the highest weight condition. They are called null states. For example, the null
states in level-1 descendants are
• As we will see next, we found the fact that these null states in W-algebra are
closely related to the singular behavior of Seiberg-Witten curve near the
punctures. That is, Toda fields whose existence is predicted by AGT relation
may in fact describe the form (or behavior) of Seiberg-Witten curve.
As usual, we compose the primary, descendant, and null fields.
• As we saw, Seiberg-Witten curve is generally represented as
and Laurent expansion near z=z0 of the coefficient function is generally
• This form is similar to Laurent expansion of W-current (i.e. W-generators)
• Also, the coefficients satisfy similar equations, except full-type puncture‟s case
This correspondence becomes exact, in some kind of „classical‟ limit:
(which is related to Dijkgraaf-Vafa‟s discussion on free fermion‟s system?)
• This fact strongly suggests that vertex operators corresponding non-full-type
punctures must be the primary fields which has null states in their descendants.
The singular behavior of SW curve is related to the null fields of W-algebra.[Kanno-Matsuo-SS-Tachikawa ‟09]
null condition
~ direction of D4 ~ direction of NS5
• If we believe this suggestion, we can conjecture the form of
momentum of Toda field in vertex operators ,
which corresponds to each kind of punctures.
• To find the form of vertex operators which have the level-1 null state, it is
useful to consider the screening operator (a special type of vertex operator)
• We can show that the state satisfies the highest weight
condition, since the screening operator commutes with all the W-generators.
(Note a strange form of a ket, since the screening operator itself has non-zero momentum.)
• This state doesn‟t vanish, if the momentum satisfies
for some j. In this case, the vertex operator has a null state at level .
The punctures on SW curve corresponds to the „degenerate‟ fields![Kanno-Matsuo-SS-Tachikawa ‟09]
• Therefore, the condition of level-1 null state becomes for some j.
• It means that the general form of mometum of Toda fields satisfying this null
state condition is .
Note that this form naturally corresponds to Young tableaux .
• More generally, the null state condition can be written as
(The factors are abbreviated, since they are only the images under Weyl transformation.)
• Moreover, from physical state condition (i.e. energy-momentum is real), we
need to choose , instead of naive generalization:
Here, is the same form of β,
is Weyl vector,
and .
The punctures on SW curve corresponds to the „degenerate‟ fields!
• We put the (primary) vertex operators at punctures, and consider
the correlation functions of them:
• In general, the following expansion is valid:
where
and for level-1 descendants,
: Shapovalov matrix
• It means that all correlation functions consist of 3-point functions and inverse
Shapovalov matrices (propagator), where the intermediate states (descendants)
can be classified by Young tableaux.
On calculation of correlation functions of 2-dim AN-1 Toda theory
descendants
primaries
In fact, we can obtain it of the factorization form of 3-point functions and inverse
Shapovalov matrices :
3-point function : We can obtain it, if one entry has a null state in level-1!
where
highest weight
~ simple punc.
On calculation of correlation functions of 2-dim AN-1 Toda theory
‟
Now we are interested in the Nekrasov‟s partition function of 4-dim SU(N)
quiver gauge theory.
It seems natural that generalized AGT relation (or AGT-W relation) clarifies
the correspondence between Nekrasov‟s function and some correlation function
of 2-dim AN-1 Toda theory:
Main difference from SU(2) case:
Not all flavor symmetries are SU(N), e.g. bifundamental flavor symmetry.
Therefore, we need the condition which restricts the d.o.f. of momentum β in
Toda vertex which corresponds to
each (kind of) puncture.
→ level-1 null state condition
[Wyllard ‟09]
[Kanno-Matsuo-SS-Tachikawa ‟09]
N-1 Cartans
SU(N)
SU(N)
SU(N)
U(1)
SU(N)
U(1) U(1)
SU(N)U(1)
SU(N)…
N-1 d.o.f.
AGT relation : 4-dim SU(N) quiver gauge and 2-dim AN-1 Toda theory
Correspondence between each kind of punctures and vertices :
we conjectured it, using level-1 null state condition for non-full-type punctures.
• full-type : correponds to SU(N) flavor symmetry (N-1 d.o.f.)
• simple-type : corresponds to U(1) flavor symmetry (1 d.o.f.)
• other types : corresponds to other flavor symmetry
The corresponding momentum is of the form
which naturally corresponds to Young tableaux .
More precisely, the momentum is , where
[Kanno-Matsuo-SS-Tachikawa ‟09]
…
…
…
…
………
Level-1 null state condition resolves the problems of AGT-W relation.
Difficulty for calculation of conformal blocks :
Here we consider the case of A2 Toda theory and W3-algebra. In usual, the
conformal blocks are written as the linear combination of
which cannot be determined by recursion formula.
However, in this case, thanks to the level-1 null state condition
we can completely determine all the conformal blocks.
Also, thanks to the level-1 null state condition, the 3-point function of primary
vertex fields can be determined completely:
Level-1 null state condition resolves the problems of AGT-W relation.
Case of SU(3) quiver gauge theory
SU(3) : already checked successfully. [Wyllard ‟09] [Mironov-Morozov ‟09]
SU(3) x … x SU(3) : We have checked successfully. [Kanno-Matsuo-SS ‟10]
SU(3) x SU(2) : We could check it, but only for restricted cases. [Kanno-Matsuo-SS ‟10]
Case of SU(4) quiver gauge theory
• In this case, there are punctures which are not full-type nor simple-type.
• So we must discuss in order to check our conjucture (of the simplest example).
• The calculation is complicated because of W4 algebra, but is mostly streightforward.
Case of SU(∞) quiver gauge theory
• In this case, we consider the system of infinitely many M5-branes, which may relate to
AdS dual system of 11-dim supergravity.
• AdS dual system is already discussed using LLM‟s droplet ansatz, which is also governed
by Toda equation. [Gaiotto-Maldacena ‟09] → subject of next section…
Our plans of current and future research on generalized AGT relation
AdS/CFT of AGT‟s system
AdS/CFT of AGT‟s system
CFT side : 4-dim SU(N≫1) quiver gauge theory and 2-dim AN-1Toda theory
• 4-dim theory is conformal.
• The system preserves eight (1/2×1/2) supersymmetries.
AdS side : the system with AdS5 and S2 factor and 1/2 BPS state of AdS7×S4
• This is nothing but the analytic continuation of LLM‟s system in M-theory.
• Moreover, when we concentrate on the neighborhood of punctures on
Seiberg-Witten curve, the system gets the
additional S1 ~ U(1) symmetry.
• According to LLM‟s discussion, such system can
be analyzed using 3-dim electricity system:
[Gaiotto-Maldacena ‟09]
[Lin-Lunin-Maldacena ‟04]
On the near horizon (dual) spacetime and its symmetry
The near horizon region of M5-branes is AdS7×S4 spacetime.
Then, what is the near horizon of intersecting M5-branes like?
0,1,2,3-direction : 4-dim quiver gauge theory lives here.
All M5-branes must be extended.
7-direction : compactification direction of M → IIA
Only M5(D4)-branes must be extended.
8,9,10-direction and 5-direction : corresponding to SU(2)×U(1) R-symmetry
No M5-branes are extended to the former, and only M5(NS5)-branes are to the
latter.
Then the result is …
(original AdS7 × S4)
r
The most general gravity solution with such symmetry is
Note that the spacetime solution is constructed from a single function
which obeys 3-dim Toda equation
(In the following, we consider the cases where the source term is non-zero.)
cf. coordinates of 11-dim spacetime:
LLM ansatz : 11-dim SUGRA solution with AdS5 x S2 factor and SUSYs
[Lin-Lunin-Maldacena ‟04]
The neighborhood of punctures : Toda equation with source term
We consider the system of N M5(D4)-branes and K M5(NS5)-branes (N≫K≫1),
and locally analyze the neighborhood of punctures (intersecting points).
• M5(NS5)-branes wrap AdS5×S1, which is conformal to R1,5.
• So, including the effect of M5(D4)-branes, the near horizon geometry is also
AdS7×S4 :
When we set the angles and (i.e. U(1) symm. for β-direction),
we can determine the correspondence to LLM ansatz coordinates as
where .
Note that D→∞ along the segment r=0 and 0≦y≦1. This means that Toda
equation must have the source term, whose charge density is constant along
the segment:
S1 S1
In this simplified situation, 11-dim spacetime has an additional U(1) symmetry.
Moreover, the analysis become much easier, if we change the variables:
Note that this transformation mixes the free and bound variables: (r, y, D) → (ρ, η, V)…
Then LLM ansatz and Toda equation becomes ( )
and
i.e.
This is nothing but the 3-dim cylindrically symmetric Laplace equation.
For simplicity, we concentrate on the neighborhood of the punctures.
ρ
η
From the U(1) symmetry of β-direction, the source must exist at ρ=0.
Near , LLM ansatz becomes more simple form (using )
Note that at (i.e. at the puncture),
• The circle is shrinking
• The circle is not shrinking.
This makes sense, only when the constant slope is integer.
In fact, this integer slopes correspond to the size of quiver gauge groups.
(→ the next page…)
For more simplicity, we concentrate on the neighborhood of the punctures.
The neighborhood of punctures : Laplace equation with source term
We consider the such distribution of source charge:
When the slope is 1, we get smooth geometry.
When the slope is k, which corresponds to the
rescale and ,
we get Ak-1 singularity at and ,
since the period of β becomes .
In general, if the slope changes by k units, we get Ak-1 singularity there.
This can be regard the flavor symmetry of
additional k fundamental hypermultiplets.
This means the source charge corresponds to
nothing but the size of quiver gauge group.
N
Near , the potential can be written as (since , )
Then we obtain
,
So the boundary condition (~ source at r=0) is
On the source term : AdS/CFT correspondence for AGT relation !
integer
x*
x
3-dim Toda equation, 2-dim Toda equation and their correspondence
3-dim Toda equation :
2-dim Toda equation (after rescaling of μ) :
Correspondence : or
[proof] The 2-dim equation (without curvature term, for simplicity) says
Therefore, under the correspondence, this 2-dim equation exactly becomes
the 3-dim equation:
differential of differential
element coordinate
To obtain the source term, we consider OPE of kinetic term of 2-dim equation
and the vertex operator :
( )
Then using the correspondence , we obtain
In massless case, (since we consider AdS/CFT correspondence).
According to our ansatz, this is of the form
where
: N elements (Weyl vector)
: k elements
Source term from 2-dim Toda equation
source??
Towards the correspondence of “source” in AdS/CFT context…?
• For full [1,…,1]-type puncture:
• For simple [N-1,1]-type puncture :
• For [l1,l2,…]-type puncture :
Conclusion
AGT relation reveals the interesting correspondence between 4-dim N=2
linear or necklace SU(2) quiver gauge theory and 2-dim Liouville theory.
We show (in part) that AGT-W relation for 4-dim linear SU(3) quiver gauge
theory and 2-dim A2 Toda theory is satisfied, by checking 1-loop factor and
some lower levels of instanton factor. Here we use effectively the level-1 null
state condition for vertices in Toda theory.
As one way to study AGT-W relation for SU(N≫1) quiver gauge theory, it
can be useful to discuss AdS/CFT correspondence. Our conjecture for general
vertices in Toda theory enables us to study this correspondence. This will be
an important future work.