bethe ansatz in sigma models · bethe ansatz in sigma models konstantin zarembo (uppsala u.)...
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Bethe ansatz in Sigma Models
Konstantin Zarembo(Uppsala U.)
“Integrability in Gauge and String Theory”, Potsdam, 24.07.2006
T. Klose, K. Z., hep-th/0603039S. Schäfer-Nameki, M. Zamaklar, K.Z., in progressT. McLoughlin, T. Klose, R. Roiban, K. Z., in progress
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Topological expansion of gauge theory
String theory
Early examples:
• 2d QCD• Matrix models
4d gauge/string duality:
• AdS/CFT correspondence
‘t Hooft’74
Brezin,Itzykson,Parisi,Zuber’78
Maldacena’97
a (theoretically) testable prediction of string theory
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AdS/CFT correspondence Maldacena’97
Gubser,Klebanov,Polyakov’98Witten’98
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Strings in AdS5xS5
Green-Schwarz-type coset sigma model on SU(2,2|4)/SO(4,1)xSO(5).
Conformal gauge is problematic:no kinetic term for fermions, no holomorphic factorization for currents, …
Light-cone gauge is OK.
Metsaev,Tseytlin’98
The action is complicated, but the model is integrable!Bena,Polchinski,Roiban’03Arutyunov,Frolov’04
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Spectrum S-matrix
(string is closed) (asymptotic states)?
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• exact only for V(x) = g d(x)
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Continuity of periodized wave function
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where
is (eigenvalue of) the S-matrix
• correct up to O(e-L/R)• works even for bound states via analytic
continuation to complex momenta
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Multy-particle states
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Bethe equations
Assumptions:• R<<L• scattering does not affect momenta of the particles• no inelastic processes
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2? 2 scattering in 2d
p1
p2
k1
k2
Energy and momentum conservation:
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I
II
Momentum conservation
Energy conservation
k1
k2
I: k1=p1, k2=p2 (transition)
II: k1=p2, k2=p1 (reflection)
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n? n scattering
2 equations for n unknowns
(n-2)-dimensional phase space
pi ki
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Unless there are extra conservation laws!
Integrability:
• No phase space:• No particle production (all 2? many
processes are kinematically forbidden)
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Factorization:
Consistency condition (Yang-Baxter equation):
1
2
3
1
2
3=
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Strategy:
• find the dispersion relation (solve the one-body problem):
• find the S-matrix (solve the two-body problem):
Bethe equations full spectrum
• find the true ground state
Integrability + Locality Bethe ansatz
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Non-linear Schrödinger model
Second quantized:
First quantized:
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S = 1 + + + + …
S-matrix
Born approximation for V(x)=2cd(x)
First iteration of Lippmann-Schwinger equation
Bethe equations:
Lieb,Liniger’63
Thacker’75
Yang’67
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• Low-energy effective theory of Heisenberg ferromagnet• Describes one-loop anomalous dimensions of operators
in N=4 SYM in the limit
• Decribes fast-moving strings on S3xR1 (SU(2) sector of string theory on AdS5xS5)
WZ term
Kruczenski’03
Landau-Lifshitz sigma-model
Minahan,Z.’02
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Exact S-matrix (of magnons):
Bethe equations:
The vacuum turns out to be unstable– there are bound states with E<0.
Klose,Z.’06
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AAF model
Alday,Arutyunov,Frolov’05
su(1|1) subsector of AdS5xS5 string theory:2 world-sheet fermions, other d.o.f. are gauge-fixed or frozen
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First order of perturbation theory
S = 1 + + …
Born approximation for Dirac equation
- rapidity
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One loop
first iteration of Lippmann-Schwinger equation
correction to the potentialdue to vacuum polarization
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p0
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p0
-µ
µ – chemical potential
µ? -8 All poles are below the real axis.
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-m
Empty Fermi sea:
E
+m
-m
E
+m
Physical vacuum:
Berezin,Sushko’65; Bergknoff,Thaker’79; Korepin’79
after computingthe S-matrix
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S = 1 + + + + + …
Empty Dirac sea:1. the potential remains local2. S-matrix is the sum of bubble diagrams
Klose, Z.’06
coincides with the S-matrix of breathers in SG
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Bethe ansatz
Im ? j=0: positive-energy states
Im ? j=p: negative-energy states
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Ground state
?
ip
0
-k+ip k+ip
- UV cutoff
Mass renormalization:
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Ground state in thermodynamic limit
• mass renormaliztion• physical spectrum• physical S-matrix
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• Weak-coupling (-1<g<1):Non-renormalizable (anomalous dimension of mass is complex)
• Strong attraction (g>1) Unstable (Energy unbounded below)
• Strong repulsion (g<-1):Spectrum consists of fermions and anti-fermionswith non-trivial scattering
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AdS/CFT
• S-matrix is virtually known• Bethe equations are nearly known
• Elementary excitations are solitons* (giant magnons)
• A lot of evidenence from SYM
Beisert’05; Janik’06; …
Kazakov,Marshakov,Minahan,Z.’04; Arutyunov,Frolov,Staudacher’04;Beisert,Kazakov,Sakai,Z.’05; Beisert,Staudacher’05; Beisert,Tseytlin’05; Hernadez,Lopez’06; …
Hofman,Maldacena’06; …
Minahan,Z.’02; Beisert,Kristjansen,Staudacher’03; Beisert,Staudacher’03; Beisert,Dippel,Staudacher’04; Staudacher’04; Rej,Serban,Staudacher’05
* which means that there are finite-size correction to the Bethe spectrum Ambjørn,Janik,Kristjansen’05
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AdS3xS1
- radial coordinate in AdS
- angle in AdS
- angle on S5
- global time
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Rigid string solution
Arutyunov,Russo,Tseytlin’03
AdS5 S5
winds k timesand rotates
winds m timesand rotates
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Quantum numbers
- AdS spin
- angular momentum on S5
- energy
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Quantum corrections
string fluctuation frequenciesExplicitly,
Park,Tirziu,Tseytlin’05
Frolov,Tseytlin’03
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Bethe equations
Classical Bethe equation
Anomaly Quantum correction to scattering phase
Hernandez,Lopez’06; Arutyunov,Frolov’06
Kazakov’04;Beisert,Kazakov,Sakai,Z.’05Beisert,Tseytlin,Z.’05; Schäfer-Nameki,Zamaklar,Z.’05
Beisert,Tseytlin’05
Kazakov,Marshakov,Minahan,Z.’04; Kazakov,Z.’04
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Internal length of the string is
Perturbative SYM regime:
(string is very long)
String and Bethe calculations agree to all orders in
Schäfer-Nameki,Zamaklar,Z.’05; Beisert,Tseytlin’05; Hernandez,Lopez’06
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Minahan,Tirziu,Tseytlin’06
Decompatification limit
string becomes infinitely long
agree
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Large winding limit
Schäfer-Nameki,Zamaklar,Z.’05
string stays finite
disagree
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What is ?
What is ?
Spectrum of AdS/CFT:
Remaining questions:
Why are they equal??