exact results for static and radiative fields ... -...
TRANSCRIPT
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EXACT RESULTS FOR STATIC AND RADIATIVE FIELDS OF A QUARK IN N=4 SUPER YANG-MILLS
Blai Garolera - Universitat de Barcelona
B. Fiol, B.G. hep-th\1106.5418 B. Fiol, B.G, A. Lewkowycz hep-th\1202.5292
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- Exact results in 4D QFT are extremely hard to obtain...
- The situation improves A LOT with additional symmetries: CFTs, SUSY, ...
N=4 SYM is both conformal and maximally supersymmetric!
- Various techniques can apply: Integrability, Localization, AdS/CFT, ...
Preview
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- Exact results in 4D QFT are extremely hard to obtain...
- The situation improves A LOT with additional symmetries: CFTs, SUSY, ...
N=4 SYM is both conformal and maximally supersymmetric!
- Various techniques can apply: Integrability, Localization, AdS/CFT, ...
Preview
![Page 4: EXACT RESULTS FOR STATIC AND RADIATIVE FIELDS ... - ffn.ub…ffn.ub.edu/bcn-encounters/wp-content/uploads/2012/10/garolera.pdf · Preview - We will focus on observables related with](https://reader033.vdocument.in/reader033/viewer/2022051921/600e268a54641351b4532232/html5/thumbnails/4.jpg)
Preview
- We will focus on observables related with external probes of N=4 SU(N) SYM.
(~idealization of QCD with two parameters: λ and N )
- First, we will use AdS/CFT to obtain results valid at large λ and to all orders in 1/N.
- Then we will use localization results to provide exact expressions, valid for all λ and N.
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Maxwell N=4 SU(N) SYM
Static particle
Accelerated particle
1|⇥x|4
q2< L(⌅x) >=
aµaµP =23q2 aµaµP = 8⇥f(�, N)
< L(⌅x) >= f(�, N)1
|⇥x|4
Preview
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f(�, N) =�
64⇥2N
L2N�1(� �
4N ) + L2N�2(� �
4N )L1
N�1(� �4N )
Maxwell N=4 SU(N) SYM
Static particle
Accelerated particle
1|⇥x|4
q2< L(⌅x) >=
aµaµP =23q2 aµaµP = 8⇥f(�, N)
< L(⌅x) >= f(�, N)1
|⇥x|4
Preview
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External probes in AdS/CFT
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UV
IR
N=4 SU(N) SYM
IIB SUGRA in AdS5xS5
z
External probes in AdS/CFT
(z=0)
(z➝∞)
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UV
IR
N=4 SU(N) SYM
IIB SUGRA in AdS5xS5
z
External probes in AdS/CFT
(z=0)
(z➝∞)
Φ(xμ, z)
<O(xμ)>
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UV
IR
N=4 SU(N) SYM
IIB SUGRA in AdS5xS5
z
External probes in AdS/CFT
(z=0)
(z➝∞)
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UV
IR
N=4 SU(N) SYM
IIB SUGRA in AdS5xS5
z
External probes in AdS/CFT
(z=0)
(z➝∞)
(z=zH)
T=TH
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UV
IR
N=4 SU(N) SYM
IIB SUGRA in AdS5xS5
z
External probes in AdS/CFT
(z=0)
(z➝∞)
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UV
IR
N=4 SU(N) SYM
IIB SUGRA in AdS5xS5
z
External probes in AdS/CFT
(z=0)
(z➝∞)
xμ(τ)
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@AdS5
AdS5
z
external color source
F1
worldsheet horizon
Poincare horizon
x
µ
(t
ret
)
P =2�
aµaµ
��
< L(⇧x) >=1
16�2 |⇧x|4
��
Vqq = � 4�2
�4�
14
⇥L
��
��ln < W� >=
External probes in AdS/CFT
There are two types of corrections: (world-sheet fluctuations) (higher genus world-sheets)
1/�
�1/N
Fundamental rep:
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@AdS5
AdS5
z
external color source
F1
worldsheet horizon
Poincare horizon
x
µ
(t
ret
)
P =2�
aµaµ
��
< L(⇧x) >=1
16�2 |⇧x|4
��
Vqq = � 4�2
�4�
14
⇥L
��
��ln < W� >=
External probes in AdS/CFT
There are two types of corrections: (world-sheet fluctuations) (higher genus world-sheets)
1/�
�1/N
Fundamental rep:
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External probes in AdS/CFT
k-symmetric rep: @AdS5
AdS5
z
external color source
Poincare horizon
worldvolume horizon
D3/D5
< L(⌅x) >Sk=1
|⇥x|4k�
�
16⇥2
�1 +
k2�
16N2
k�
�
2⇥
�1 +
k2�
16N2P = aµaµ
ln < W (�) >=k�
�
2
�1 +
k2�
16N2+ 2N sinh�1 k
��
4N
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Exact results for external probes
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Exact results for external probes
SCT(E) A.C.
SCT(L)
r1 = R
r1 = 0
x
0
x
1
< W| >= 1 < W� >�= 1
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Exact results for external probes
SCT(E) A.C.
SCT(L)
r1 = R
r1 = 0
x
0
x
1
< W| >= 1 < W� >�= 1
Conformal anomaly!
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Exact results for external probes
The anomaly is localized in a single point in space-time
It is perturbatively captured by a matrix model:
< W⇥ >=1N
L1N�1
�� �
4N
⇥e
�8N
By means of localization techniques, it was proved that this result is correct and exact
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Exact results for external probes
The two-point function of a circular Wilson loop and a chiral primary operator can also be computed with a matrix model
< W (⇥)�O2 >=⌅
2�
4N3
⇤L2
N�1
�� �
4N
⇥+ L2
N�2
�� �
4N
⇥⌅e
�8N
and from this we can extract the one-point function of the chiral primary operator in the presence of the probe
< O2 >J=< WO2 >
< W >=⇤
2�
4N2
L2N�1(� �
4N ) + L2N�2(� �
4N )L1
N�1(� �4N )
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A key observation for our problem at hand is that in N=4 SYM, the Lagrangian and the stress-energy tensor belong to the same short multiplet, the supercurrent multiplet:
Exact results for external probes
O2 = Tr��{I�J}
⇥L � Q4O2 Tµ⇥ � Q2Q2O2
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A key observation for our problem at hand is that in N=4 SYM, the Lagrangian and the stress-energy tensor belong to the same short multiplet, the supercurrent multiplet:
Exact results for external probes
O2 = Tr��{I�J}
⇥L � Q4O2 Tµ⇥ � Q2Q2O2
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A key observation for our problem at hand is that in N=4 SYM, the Lagrangian and the stress-energy tensor belong to the same short multiplet, the supercurrent multiplet:
Exact results for external probes
O2 = Tr��{I�J}
⇥L � Q4O2 Tµ⇥ � Q2Q2O2
< L(�x) >�=�
64⇥2N
L2N�1(� �
4N ) + L2N�2(� �
4N )L1
N�1(� �4N )
1|�x|4
P =�
8⇥N
L2N�1(� �
4N ) + L2N�2(� �
4N )L1
N�1(� �4N )
1R2
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QFT results EXACT for any λ and N.
If we take the large λ and large N limit we precisely recover our AdS/CFT results obtained with D3-branes, for k=1!
Exact results for external probes
These are very precise tests of the AdS/CFT correspondence, valid to all orders in 1/N!
Setting k=1 in our D-brane computation is not justified a priori... but it works! WHY?