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Aspects of the AdS/ CFT dictionary, II David Berenstein, UCSB, Durban, 1-15-19 Research supported by

Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

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Page 1: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Aspects of the AdS/CFT dictionary, II

David Berenstein, UCSB,Durban, 1-15-19

Research supported by

Page 2: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

AdS/CFT correspondence

Quantum gravity can be equivalent to quantum field theory in fewer dimensions.

Page 3: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Simplest (original) example

N = 4SYM on S3 ⇥ R$Type IIB superstring on (global) AdS5 ⇥ S5

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Original Maldacena paper hep-th/9711200

Page 4: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

We want to explore CFT at large values of R -large ‘t Hooft

coupling- but with g fixed and small.

AdS/CFT is a strong weak-coupling duality for the

‘t Hooft coupling constant.

Isometries Global symmetries

R4 g2Y MN

Flux = N Gauge group U(N)

State State

AdS CFT

Basic dictionary for simplest case

Standard Table

Page 5: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Field contentZ, Z,�i=1,...4, Aµ

J=1,...4↵ , ↵

J=1,...4<latexit sha1_base64="D02ycfgCBAT+iB3lYvs/3MPN0yM=">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</latexit><latexit sha1_base64="D02ycfgCBAT+iB3lYvs/3MPN0yM=">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</latexit><latexit sha1_base64="D02ycfgCBAT+iB3lYvs/3MPN0yM=">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</latexit><latexit sha1_base64="D02ycfgCBAT+iB3lYvs/3MPN0yM=">AAACU3icdVHLSgMxFM2M7/qqunQTLIKLUmbqYHUh+NiIKwVbxU4d7qRpG5uZCUlGKEP/UQQX/ogbF5ppK1jRCyGHc8+5SU5CwZnSjvNm2TOzc/MLi0uF5ZXVtfXixmZDJakktE4Snsi7EBTlLKZ1zTSnd0JSiEJOb8P+ed6/faJSsSS+0QNBWxF0Y9ZhBLShguLjfRn7IUic76LHgowduwa2E62wNyzj08CPUt8v+EKxwAcuevCQXU5rRgNywUOWk3gsGwbTuqBYcipHhwdV7wA7FcepuVU3B9Wat+9h1zB5ldCkroLii7GSNKKxJhyUarqO0K0MpGaE02HBTxUVQPrQpU0DY4ioamWjTIZ41zBt3EmkWbHGI/anI4NIqUEUGmUEuqd+93Lyr14z1Z3DVsZikWoak/FBnZRjneA8YNxmkhLNBwYAkczcFZMeSCDafEPBhPD9Uvw/aFQrrsHXXunkbBLHItpGO2gPuaiGTtAFukJ1RNAzekefFrJerQ/btmfHUtuaeLbQVNmrX9lXsJE=</latexit>

Z is highest weight of SO(6)~SU(4) in 6 rep.Bosons have dim=1, fermions = 3/2

All in adjoint of SU(N) (need to track extra gauge indices)

Page 6: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Single particle state = traceBPS particle maximizes SO(6) R-charge given dimension

This is highest weight state of SO(6) in a symmetric traceless tensor rep.Has a lot of null descendants, so it is massless in 10DCan’t be lifted: does not allow anomalous dimension.

Tr(Zn)|n�2,...<latexit sha1_base64="bSv7JiK7qZzAvesk8k0YvWdQM9E=">AAACA3icdVDLSgMxFM3UV62vqjvdBItQQcrMWNq6K7pxWaEvbMchk6ZtaCYzJhmhjAU3/oobF4q49Sfc+TdmbAUVPRA4nHMPN/d4IaNSmea7kZqbX1hcSi9nVlbX1jeym1tNGUQCkwYOWCDaHpKEUU4aiipG2qEgyPcYaXmj08RvXRMhacDrahwSx0cDTvsUI6UlN7tTF3l4cckPbtyYdwfkCtqHsNsLlJy42ZxZOK6U7GIJmgXTLFu2lRC7XDwqQksrCXJghpqbfdNBHPmEK8yQlB3LDJUTI6EoZmSS6UaShAiP0IB0NOXIJ9KJP2+YwH2t9GA/EPpxBT/V74kY+VKOfU9P+kgN5W8vEf/yOpHqV5yY8jBShOPpon7EoApgUgjsUUGwYmNNEBZU/xXiIRIIK11bRpfwdSn8nzTtgqX5eTFXPZnVkQa7YA/kgQXKoArOQA00AAa34B48gifjzngwno2X6WjKmGW2wQ8Yrx+Wmpbc</latexit><latexit sha1_base64="bSv7JiK7qZzAvesk8k0YvWdQM9E=">AAACA3icdVDLSgMxFM3UV62vqjvdBItQQcrMWNq6K7pxWaEvbMchk6ZtaCYzJhmhjAU3/oobF4q49Sfc+TdmbAUVPRA4nHMPN/d4IaNSmea7kZqbX1hcSi9nVlbX1jeym1tNGUQCkwYOWCDaHpKEUU4aiipG2qEgyPcYaXmj08RvXRMhacDrahwSx0cDTvsUI6UlN7tTF3l4cckPbtyYdwfkCtqHsNsLlJy42ZxZOK6U7GIJmgXTLFu2lRC7XDwqQksrCXJghpqbfdNBHPmEK8yQlB3LDJUTI6EoZmSS6UaShAiP0IB0NOXIJ9KJP2+YwH2t9GA/EPpxBT/V74kY+VKOfU9P+kgN5W8vEf/yOpHqV5yY8jBShOPpon7EoApgUgjsUUGwYmNNEBZU/xXiIRIIK11bRpfwdSn8nzTtgqX5eTFXPZnVkQa7YA/kgQXKoArOQA00AAa34B48gifjzngwno2X6WjKmGW2wQ8Yrx+Wmpbc</latexit><latexit sha1_base64="bSv7JiK7qZzAvesk8k0YvWdQM9E=">AAACA3icdVDLSgMxFM3UV62vqjvdBItQQcrMWNq6K7pxWaEvbMchk6ZtaCYzJhmhjAU3/oobF4q49Sfc+TdmbAUVPRA4nHMPN/d4IaNSmea7kZqbX1hcSi9nVlbX1jeym1tNGUQCkwYOWCDaHpKEUU4aiipG2qEgyPcYaXmj08RvXRMhacDrahwSx0cDTvsUI6UlN7tTF3l4cckPbtyYdwfkCtqHsNsLlJy42ZxZOK6U7GIJmgXTLFu2lRC7XDwqQksrCXJghpqbfdNBHPmEK8yQlB3LDJUTI6EoZmSS6UaShAiP0IB0NOXIJ9KJP2+YwH2t9GA/EPpxBT/V74kY+VKOfU9P+kgN5W8vEf/yOpHqV5yY8jBShOPpon7EoApgUgjsUUGwYmNNEBZU/xXiIRIIK11bRpfwdSn8nzTtgqX5eTFXPZnVkQa7YA/kgQXKoArOQA00AAa34B48gifjzngwno2X6WjKmGW2wQ8Yrx+Wmpbc</latexit><latexit sha1_base64="bSv7JiK7qZzAvesk8k0YvWdQM9E=">AAACA3icdVDLSgMxFM3UV62vqjvdBItQQcrMWNq6K7pxWaEvbMchk6ZtaCYzJhmhjAU3/oobF4q49Sfc+TdmbAUVPRA4nHMPN/d4IaNSmea7kZqbX1hcSi9nVlbX1jeym1tNGUQCkwYOWCDaHpKEUU4aiipG2qEgyPcYaXmj08RvXRMhacDrahwSx0cDTvsUI6UlN7tTF3l4cckPbtyYdwfkCtqHsNsLlJy42ZxZOK6U7GIJmgXTLFu2lRC7XDwqQksrCXJghpqbfdNBHPmEK8yQlB3LDJUTI6EoZmSS6UaShAiP0IB0NOXIJ9KJP2+YwH2t9GA/EPpxBT/V74kY+VKOfU9P+kgN5W8vEf/yOpHqV5yY8jBShOPpon7EoApgUgjsUUGwYmNNEBZU/xXiIRIIK11bRpfwdSn8nzTtgqX5eTFXPZnVkQa7YA/kgQXKoArOQA00AAa34B48gifjzngwno2X6WjKmGW2wQ8Yrx+Wmpbc</latexit>

THE FACT THAT IT STARTS AT n=2 is that the spin of particle in 10D is 2

Page 7: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Convenient to expand Near BPS state

X

k

f(k)Tr(Zk�iZJ�k�i0)

<latexit sha1_base64="1IEKM8ggKUesZ+JeCujQkJhJBHQ=">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</latexit><latexit sha1_base64="1IEKM8ggKUesZ+JeCujQkJhJBHQ=">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</latexit><latexit sha1_base64="1IEKM8ggKUesZ+JeCujQkJhJBHQ=">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</latexit><latexit sha1_base64="1IEKM8ggKUesZ+JeCujQkJhJBHQ=">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</latexit>

Interpreted as defects moving in a sea of Z

Anomalous dimensions can be computed perturbatively and thegap scales as powers of 1/J

Page 8: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

The interaction term

∼g2Y MTr([Z,φj][Z,φj])

will make the defects hop to the left or right in theoperator.

The idea now is to interpret the position of the defectsin between the Z as a lattice. The number of sites isof order J ∼

√N , so in the large N limit we obtain a

continuum theory.

We need to rewrite the states in a momentum basis,so we apply position dependent phases for inserting thesame defect at different positions.

20

The interaction term + planarity

Defects hop in between Z:nearest neighbor hopping.

Can be mapped to spin chains.

Page 9: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Berenstein, Maldacena, Nastase hep-th/0202021 (BMN)

Minahan, Zarembo hep-th/0212208 (Bethe Ansatz)

Beisert, Staudacher, hep-th/0307042 (USp(2,2|4) integrability)(Used all the Lipatov SL(2) anomalous dimensions from QCD)

Spin chain program

Page 10: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Gave rise to integrability program for strings in AdS x S

Interpolation between weak and strong coupling *Solved (Y system) *.

* Integrability not proved: it is a working assumption. Checked to 5 (or 6) loop order

of some anomalous dimensions

Page 11: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Covers energies up to

o(pN)

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Page 12: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Extended objects: D-branes

There exist half BPS states that are D-brane like extended objects.

These are called giant and dual giant gravitons.

McGreevy, Susskind, Toumbas hep-th/0003075Grisaru, Myers, Tajford hep-th/0008015

Hashimoto, Hirano, Itzhaki hep-th/0008016

Page 13: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Simple description. Write the 5 sphere in cartesian coordinates.

zz +4X

i=1

y2i = 1<latexit sha1_base64="2ZQovfQXXK9s8Cn/AFbm3OG8DDI=">AAACCHicdZDLSsNAFIYnXmu9RV26cLAIglCSUtGNUHTjsoK9QJuGyXTSDp1MwsxESEOXbnwVNy4UcesjuPNtnLQpqOgPAz/fOYcz5/ciRqWyrE9jYXFpeWW1sFZc39jc2jZ3dpsyjAUmDRyyULQ9JAmjnDQUVYy0I0FQ4DHS8kZXWb11R4SkIb9VSUScAA049SlGSiPXPBjDrocEHMMT2JVx4Kb0wp70qjDpVVxtXbNklU+tTNAqW3OTEzsnJZCr7pof3X6I44BwhRmSsmNbkXJSJBTFjEyK3ViSCOERGpCOthwFRDrp9JAJPNKkD/1Q6McVnNLvEykKpEwCT3cGSA3l71oG/6p1YuWfOynlUawIx7NFfsygCmGWCuxTQbBiiTYIC6r/CvEQCYSVzq6oQ5hfCv83zUrZ1v6mWqpd5nEUwD44BMfABmegBq5BHTQABvfgETyDF+PBeDJejbdZ64KRz+yBHzLevwDQTZfr</latexit><latexit sha1_base64="2ZQovfQXXK9s8Cn/AFbm3OG8DDI=">AAACCHicdZDLSsNAFIYnXmu9RV26cLAIglCSUtGNUHTjsoK9QJuGyXTSDp1MwsxESEOXbnwVNy4UcesjuPNtnLQpqOgPAz/fOYcz5/ciRqWyrE9jYXFpeWW1sFZc39jc2jZ3dpsyjAUmDRyyULQ9JAmjnDQUVYy0I0FQ4DHS8kZXWb11R4SkIb9VSUScAA049SlGSiPXPBjDrocEHMMT2JVx4Kb0wp70qjDpVVxtXbNklU+tTNAqW3OTEzsnJZCr7pof3X6I44BwhRmSsmNbkXJSJBTFjEyK3ViSCOERGpCOthwFRDrp9JAJPNKkD/1Q6McVnNLvEykKpEwCT3cGSA3l71oG/6p1YuWfOynlUawIx7NFfsygCmGWCuxTQbBiiTYIC6r/CvEQCYSVzq6oQ5hfCv83zUrZ1v6mWqpd5nEUwD44BMfABmegBq5BHTQABvfgETyDF+PBeDJejbdZ64KRz+yBHzLevwDQTZfr</latexit><latexit sha1_base64="2ZQovfQXXK9s8Cn/AFbm3OG8DDI=">AAACCHicdZDLSsNAFIYnXmu9RV26cLAIglCSUtGNUHTjsoK9QJuGyXTSDp1MwsxESEOXbnwVNy4UcesjuPNtnLQpqOgPAz/fOYcz5/ciRqWyrE9jYXFpeWW1sFZc39jc2jZ3dpsyjAUmDRyyULQ9JAmjnDQUVYy0I0FQ4DHS8kZXWb11R4SkIb9VSUScAA049SlGSiPXPBjDrocEHMMT2JVx4Kb0wp70qjDpVVxtXbNklU+tTNAqW3OTEzsnJZCr7pof3X6I44BwhRmSsmNbkXJSJBTFjEyK3ViSCOERGpCOthwFRDrp9JAJPNKkD/1Q6McVnNLvEykKpEwCT3cGSA3l71oG/6p1YuWfOynlUawIx7NFfsygCmGWCuxTQbBiiTYIC6r/CvEQCYSVzq6oQ5hfCv83zUrZ1v6mWqpd5nEUwD44BMfABmegBq5BHTQABvfgETyDF+PBeDJejbdZ64KRz+yBHzLevwDQTZfr</latexit><latexit sha1_base64="2ZQovfQXXK9s8Cn/AFbm3OG8DDI=">AAACCHicdZDLSsNAFIYnXmu9RV26cLAIglCSUtGNUHTjsoK9QJuGyXTSDp1MwsxESEOXbnwVNy4UcesjuPNtnLQpqOgPAz/fOYcz5/ciRqWyrE9jYXFpeWW1sFZc39jc2jZ3dpsyjAUmDRyyULQ9JAmjnDQUVYy0I0FQ4DHS8kZXWb11R4SkIb9VSUScAA049SlGSiPXPBjDrocEHMMT2JVx4Kb0wp70qjDpVVxtXbNklU+tTNAqW3OTEzsnJZCr7pof3X6I44BwhRmSsmNbkXJSJBTFjEyK3ViSCOERGpCOthwFRDrp9JAJPNKkD/1Q6McVnNLvEykKpEwCT3cGSA3l71oG/6p1YuWfOynlUawIx7NFfsygCmGWCuxTQbBiiTYIC6r/CvEQCYSVzq6oQ5hfCv83zUrZ1v6mWqpd5nEUwD44BMfABmegBq5BHTQABvfgETyDF+PBeDJejbdZ64KRz+yBHzLevwDQTZfr</latexit>

z(t) = z0 exp(it)<latexit sha1_base64="A/UxrIlG2UqeY/zKDZBlrRddy0o=">AAAB/XicdVBNSwJRFH1jX2Zf9rFr80gC3cjMJGqLQGrT0iA10GF483zqwzcfvHcnUpH+SpsWRbTtf7Tr3/RGDSrqwIXDOfdy7z1eJLgC0/wwUkvLK6tr6fXMxubW9k52d6+pwlhS1qChCOWNRxQTPGAN4CDYTSQZ8T3BWt7wIvFbt0wqHgbXMIqY45N+wHucEtCSmz0Y56GAz/DYNXGH3UV5jqHgZnNm8bRatktlbBZNs2LZVkLsSumkhC2tJMihBepu9r3TDWnsswCoIEq1LTMCZ0IkcCrYNNOJFYsIHZI+a2saEJ8pZzK7foqPtdLFvVDqCgDP1O8TE+IrNfI93ekTGKjfXiL+5bVj6FWdCQ+iGFhA54t6scAQ4iQK3OWSURAjTQiVXN+K6YBIQkEHltEhfH2K/ydNu2hpflXK1c4XcaTRITpCeWShCqqhS1RHDUTRGD2gJ/Rs3BuPxovxOm9NGYuZffQDxtsn4BeTkQ==</latexit><latexit sha1_base64="A/UxrIlG2UqeY/zKDZBlrRddy0o=">AAAB/XicdVBNSwJRFH1jX2Zf9rFr80gC3cjMJGqLQGrT0iA10GF483zqwzcfvHcnUpH+SpsWRbTtf7Tr3/RGDSrqwIXDOfdy7z1eJLgC0/wwUkvLK6tr6fXMxubW9k52d6+pwlhS1qChCOWNRxQTPGAN4CDYTSQZ8T3BWt7wIvFbt0wqHgbXMIqY45N+wHucEtCSmz0Y56GAz/DYNXGH3UV5jqHgZnNm8bRatktlbBZNs2LZVkLsSumkhC2tJMihBepu9r3TDWnsswCoIEq1LTMCZ0IkcCrYNNOJFYsIHZI+a2saEJ8pZzK7foqPtdLFvVDqCgDP1O8TE+IrNfI93ekTGKjfXiL+5bVj6FWdCQ+iGFhA54t6scAQ4iQK3OWSURAjTQiVXN+K6YBIQkEHltEhfH2K/ydNu2hpflXK1c4XcaTRITpCeWShCqqhS1RHDUTRGD2gJ/Rs3BuPxovxOm9NGYuZffQDxtsn4BeTkQ==</latexit><latexit sha1_base64="A/UxrIlG2UqeY/zKDZBlrRddy0o=">AAAB/XicdVBNSwJRFH1jX2Zf9rFr80gC3cjMJGqLQGrT0iA10GF483zqwzcfvHcnUpH+SpsWRbTtf7Tr3/RGDSrqwIXDOfdy7z1eJLgC0/wwUkvLK6tr6fXMxubW9k52d6+pwlhS1qChCOWNRxQTPGAN4CDYTSQZ8T3BWt7wIvFbt0wqHgbXMIqY45N+wHucEtCSmz0Y56GAz/DYNXGH3UV5jqHgZnNm8bRatktlbBZNs2LZVkLsSumkhC2tJMihBepu9r3TDWnsswCoIEq1LTMCZ0IkcCrYNNOJFYsIHZI+a2saEJ8pZzK7foqPtdLFvVDqCgDP1O8TE+IrNfI93ekTGKjfXiL+5bVj6FWdCQ+iGFhA54t6scAQ4iQK3OWSURAjTQiVXN+K6YBIQkEHltEhfH2K/ydNu2hpflXK1c4XcaTRITpCeWShCqqhS1RHDUTRGD2gJ/Rs3BuPxovxOm9NGYuZffQDxtsn4BeTkQ==</latexit><latexit sha1_base64="A/UxrIlG2UqeY/zKDZBlrRddy0o=">AAAB/XicdVBNSwJRFH1jX2Zf9rFr80gC3cjMJGqLQGrT0iA10GF483zqwzcfvHcnUpH+SpsWRbTtf7Tr3/RGDSrqwIXDOfdy7z1eJLgC0/wwUkvLK6tr6fXMxubW9k52d6+pwlhS1qChCOWNRxQTPGAN4CDYTSQZ8T3BWt7wIvFbt0wqHgbXMIqY45N+wHucEtCSmz0Y56GAz/DYNXGH3UV5jqHgZnNm8bRatktlbBZNs2LZVkLsSumkhC2tJMihBepu9r3TDWnsswCoIEq1LTMCZ0IkcCrYNNOJFYsIHZI+a2saEJ8pZzK7foqPtdLFvVDqCgDP1O8TE+IrNfI93ekTGKjfXiL+5bVj6FWdCQ+iGFhA54t6scAQ4iQK3OWSURAjTQiVXN+K6YBIQkEHltEhfH2K/ydNu2hpflXK1c4XcaTRITpCeWShCqqhS1RHDUTRGD2gJ/Rs3BuPxovxOm9NGYuZffQDxtsn4BeTkQ==</latexit>

Consider a 3-sphere at fixed z and move it as follows in time

Sits at origin of global AdS coordinates.

z = cos(✓) exp(i�)<latexit sha1_base64="ErrbacEToOr+YriCTWQOgIoLKoI=">AAACBXicdVA9SwNBEN3zM8avqKUWi0GITbg7Q6KFELSxVDAmkAthbzMxS/Y+2J0T42Fj41+xsVDE1v9g579xTyOo6IOBx3szzMzzYyk02vabNTE5NT0zm5vLzy8sLi0XVlbPdJQoDg0eyUi1fKZBihAaKFBCK1bAAl9C0x8eZn7zApQWUXiKoxg6ATsPRV9whkbqFjau6D71eKRLHg4A2Tb14DIuCS8eiO1uoWiX93arbqVK7bJt1xzXyYhbq+xUqGOUDEUyxnG38Or1Ip4EECKXTOu2Y8fYSZlCwSVc571EQ8z4kJ1D29CQBaA76ccX13TLKD3aj5SpEOmH+n0iZYHWo8A3nQHDgf7tZeJfXjvB/m4nFWGcIIT8c1E/kRQjmkVCe0IBRzkyhHElzK2UD5hiHE1weRPC16f0f3Lmlh3DTyrF+sE4jhxZJ5ukRBxSI3VyRI5Jg3ByQ+7IA3m0bq1768l6/mydsMYza+QHrJd3zQCXgA==</latexit><latexit sha1_base64="ErrbacEToOr+YriCTWQOgIoLKoI=">AAACBXicdVA9SwNBEN3zM8avqKUWi0GITbg7Q6KFELSxVDAmkAthbzMxS/Y+2J0T42Fj41+xsVDE1v9g579xTyOo6IOBx3szzMzzYyk02vabNTE5NT0zm5vLzy8sLi0XVlbPdJQoDg0eyUi1fKZBihAaKFBCK1bAAl9C0x8eZn7zApQWUXiKoxg6ATsPRV9whkbqFjau6D71eKRLHg4A2Tb14DIuCS8eiO1uoWiX93arbqVK7bJt1xzXyYhbq+xUqGOUDEUyxnG38Or1Ip4EECKXTOu2Y8fYSZlCwSVc571EQ8z4kJ1D29CQBaA76ccX13TLKD3aj5SpEOmH+n0iZYHWo8A3nQHDgf7tZeJfXjvB/m4nFWGcIIT8c1E/kRQjmkVCe0IBRzkyhHElzK2UD5hiHE1weRPC16f0f3Lmlh3DTyrF+sE4jhxZJ5ukRBxSI3VyRI5Jg3ByQ+7IA3m0bq1768l6/mydsMYza+QHrJd3zQCXgA==</latexit><latexit sha1_base64="ErrbacEToOr+YriCTWQOgIoLKoI=">AAACBXicdVA9SwNBEN3zM8avqKUWi0GITbg7Q6KFELSxVDAmkAthbzMxS/Y+2J0T42Fj41+xsVDE1v9g579xTyOo6IOBx3szzMzzYyk02vabNTE5NT0zm5vLzy8sLi0XVlbPdJQoDg0eyUi1fKZBihAaKFBCK1bAAl9C0x8eZn7zApQWUXiKoxg6ATsPRV9whkbqFjau6D71eKRLHg4A2Tb14DIuCS8eiO1uoWiX93arbqVK7bJt1xzXyYhbq+xUqGOUDEUyxnG38Or1Ip4EECKXTOu2Y8fYSZlCwSVc571EQ8z4kJ1D29CQBaA76ccX13TLKD3aj5SpEOmH+n0iZYHWo8A3nQHDgf7tZeJfXjvB/m4nFWGcIIT8c1E/kRQjmkVCe0IBRzkyhHElzK2UD5hiHE1weRPC16f0f3Lmlh3DTyrF+sE4jhxZJ5ukRBxSI3VyRI5Jg3ByQ+7IA3m0bq1768l6/mydsMYza+QHrJd3zQCXgA==</latexit><latexit sha1_base64="ErrbacEToOr+YriCTWQOgIoLKoI=">AAACBXicdVA9SwNBEN3zM8avqKUWi0GITbg7Q6KFELSxVDAmkAthbzMxS/Y+2J0T42Fj41+xsVDE1v9g579xTyOo6IOBx3szzMzzYyk02vabNTE5NT0zm5vLzy8sLi0XVlbPdJQoDg0eyUi1fKZBihAaKFBCK1bAAl9C0x8eZn7zApQWUXiKoxg6ATsPRV9whkbqFjau6D71eKRLHg4A2Tb14DIuCS8eiO1uoWiX93arbqVK7bJt1xzXyYhbq+xUqGOUDEUyxnG38Or1Ip4EECKXTOu2Y8fYSZlCwSVc571EQ8z4kJ1D29CQBaA76ccX13TLKD3aj5SpEOmH+n0iZYHWo8A3nQHDgf7tZeJfXjvB/m4nFWGcIIT8c1E/kRQjmkVCe0IBRzkyhHElzK2UD5hiHE1weRPC16f0f3Lmlh3DTyrF+sE4jhxZJ5ukRBxSI3VyRI5Jg3ByQ+7IA3m0bq1768l6/mydsMYza+QHrJd3zQCXgA==</latexit>

� = 1<latexit sha1_base64="Qw7ebSUcFqFlDjRe39TChl9xSuw=">AAAB83icdVDLSsNAFJ34rPVVdelmsAiuSlJDWxdC0Y3LCvYBTSiT6aQdOpmEmRuhhP6GGxeKuPVn3Pk3TtoKKnpg4HDOPdw7J0gE12DbH9bK6tr6xmZhq7i9s7u3Xzo47Og4VZS1aSxi1QuIZoJL1gYOgvUSxUgUCNYNJte5371nSvNY3sE0YX5ERpKHnBIwkucNY8BeMub40hmUynblolGrujVsV2y77lSdnFTr7rmLHaPkKKMlWoPSu4nTNGISqCBa9x07AT8jCjgVbFb0Us0SQidkxPqGShIx7Wfzm2f41ChDHMbKPAl4rn5PZCTSehoFZjIiMNa/vVz8y+unEDb8jMskBSbpYlGYCgwxzgvAQ64YBTE1hFDFza2YjokiFExNRVPC10/x/6RTrTiG37rl5tWyjgI6RifoDDmojproBrVQG1GUoAf0hJ6t1Hq0XqzXxeiKtcwcoR+w3j4BM8eRIg==</latexit><latexit sha1_base64="Qw7ebSUcFqFlDjRe39TChl9xSuw=">AAAB83icdVDLSsNAFJ34rPVVdelmsAiuSlJDWxdC0Y3LCvYBTSiT6aQdOpmEmRuhhP6GGxeKuPVn3Pk3TtoKKnpg4HDOPdw7J0gE12DbH9bK6tr6xmZhq7i9s7u3Xzo47Og4VZS1aSxi1QuIZoJL1gYOgvUSxUgUCNYNJte5371nSvNY3sE0YX5ERpKHnBIwkucNY8BeMub40hmUynblolGrujVsV2y77lSdnFTr7rmLHaPkKKMlWoPSu4nTNGISqCBa9x07AT8jCjgVbFb0Us0SQidkxPqGShIx7Wfzm2f41ChDHMbKPAl4rn5PZCTSehoFZjIiMNa/vVz8y+unEDb8jMskBSbpYlGYCgwxzgvAQ64YBTE1hFDFza2YjokiFExNRVPC10/x/6RTrTiG37rl5tWyjgI6RifoDDmojproBrVQG1GUoAf0hJ6t1Hq0XqzXxeiKtcwcoR+w3j4BM8eRIg==</latexit><latexit sha1_base64="Qw7ebSUcFqFlDjRe39TChl9xSuw=">AAAB83icdVDLSsNAFJ34rPVVdelmsAiuSlJDWxdC0Y3LCvYBTSiT6aQdOpmEmRuhhP6GGxeKuPVn3Pk3TtoKKnpg4HDOPdw7J0gE12DbH9bK6tr6xmZhq7i9s7u3Xzo47Og4VZS1aSxi1QuIZoJL1gYOgvUSxUgUCNYNJte5371nSvNY3sE0YX5ERpKHnBIwkucNY8BeMub40hmUynblolGrujVsV2y77lSdnFTr7rmLHaPkKKMlWoPSu4nTNGISqCBa9x07AT8jCjgVbFb0Us0SQidkxPqGShIx7Wfzm2f41ChDHMbKPAl4rn5PZCTSehoFZjIiMNa/vVz8y+unEDb8jMskBSbpYlGYCgwxzgvAQ64YBTE1hFDFza2YjokiFExNRVPC10/x/6RTrTiG37rl5tWyjgI6RifoDDmojproBrVQG1GUoAf0hJ6t1Hq0XqzXxeiKtcwcoR+w3j4BM8eRIg==</latexit><latexit sha1_base64="Qw7ebSUcFqFlDjRe39TChl9xSuw=">AAAB83icdVDLSsNAFJ34rPVVdelmsAiuSlJDWxdC0Y3LCvYBTSiT6aQdOpmEmRuhhP6GGxeKuPVn3Pk3TtoKKnpg4HDOPdw7J0gE12DbH9bK6tr6xmZhq7i9s7u3Xzo47Og4VZS1aSxi1QuIZoJL1gYOgvUSxUgUCNYNJte5371nSvNY3sE0YX5ERpKHnBIwkucNY8BeMub40hmUynblolGrujVsV2y77lSdnFTr7rmLHaPkKKMlWoPSu4nTNGISqCBa9x07AT8jCjgVbFb0Us0SQidkxPqGShIx7Wfzm2f41ChDHMbKPAl4rn5PZCTSehoFZjIiMNa/vVz8y+unEDb8jMskBSbpYlGYCgwxzgvAQ64YBTE1hFDFza2YjokiFExNRVPC10/x/6RTrTiG37rl5tWyjgI6RifoDDmojproBrVQG1GUoAf0hJ6t1Hq0XqzXxeiKtcwcoR+w3j4BM8eRIg==</latexit>

⇢ = 0<latexit sha1_base64="3UAsdzuJ9FQ9O/8QIOSp6bI+u4E=">AAAB7XicdVDLSgMxFM3UV62vqks3wSK4Kpk6tHUhFN24rGAf0A4lk2ba2EwyJBmhDP0HNy4Ucev/uPNvzLQVVPTAhcM593LvPUHMmTYIfTi5ldW19Y38ZmFre2d3r7h/0NYyUYS2iORSdQOsKWeCtgwznHZjRXEUcNoJJleZ37mnSjMpbs00pn6ER4KFjGBjpXZfjeUFGhRLqHxer1a8KkRlhGpuxc1IpeadedC1SoYSWKI5KL73h5IkERWGcKx1z0Wx8VOsDCOczgr9RNMYkwke0Z6lAkdU++n82hk8scoQhlLZEgbO1e8TKY60nkaB7YywGevfXib+5fUSE9b9lIk4MVSQxaIw4dBImL0Oh0xRYvjUEkwUs7dCMsYKE2MDKtgQvj6F/5N2pexafuOVGpfLOPLgCByDU+CCGmiAa9AELUDAHXgAT+DZkc6j8+K8LlpzznLmEPyA8/YJcl2PCg==</latexit><latexit sha1_base64="3UAsdzuJ9FQ9O/8QIOSp6bI+u4E=">AAAB7XicdVDLSgMxFM3UV62vqks3wSK4Kpk6tHUhFN24rGAf0A4lk2ba2EwyJBmhDP0HNy4Ucev/uPNvzLQVVPTAhcM593LvPUHMmTYIfTi5ldW19Y38ZmFre2d3r7h/0NYyUYS2iORSdQOsKWeCtgwznHZjRXEUcNoJJleZ37mnSjMpbs00pn6ER4KFjGBjpXZfjeUFGhRLqHxer1a8KkRlhGpuxc1IpeadedC1SoYSWKI5KL73h5IkERWGcKx1z0Wx8VOsDCOczgr9RNMYkwke0Z6lAkdU++n82hk8scoQhlLZEgbO1e8TKY60nkaB7YywGevfXib+5fUSE9b9lIk4MVSQxaIw4dBImL0Oh0xRYvjUEkwUs7dCMsYKE2MDKtgQvj6F/5N2pexafuOVGpfLOPLgCByDU+CCGmiAa9AELUDAHXgAT+DZkc6j8+K8LlpzznLmEPyA8/YJcl2PCg==</latexit><latexit sha1_base64="3UAsdzuJ9FQ9O/8QIOSp6bI+u4E=">AAAB7XicdVDLSgMxFM3UV62vqks3wSK4Kpk6tHUhFN24rGAf0A4lk2ba2EwyJBmhDP0HNy4Ucev/uPNvzLQVVPTAhcM593LvPUHMmTYIfTi5ldW19Y38ZmFre2d3r7h/0NYyUYS2iORSdQOsKWeCtgwznHZjRXEUcNoJJleZ37mnSjMpbs00pn6ER4KFjGBjpXZfjeUFGhRLqHxer1a8KkRlhGpuxc1IpeadedC1SoYSWKI5KL73h5IkERWGcKx1z0Wx8VOsDCOczgr9RNMYkwke0Z6lAkdU++n82hk8scoQhlLZEgbO1e8TKY60nkaB7YywGevfXib+5fUSE9b9lIk4MVSQxaIw4dBImL0Oh0xRYvjUEkwUs7dCMsYKE2MDKtgQvj6F/5N2pexafuOVGpfLOPLgCByDU+CCGmiAa9AELUDAHXgAT+DZkc6j8+K8LlpzznLmEPyA8/YJcl2PCg==</latexit><latexit sha1_base64="3UAsdzuJ9FQ9O/8QIOSp6bI+u4E=">AAAB7XicdVDLSgMxFM3UV62vqks3wSK4Kpk6tHUhFN24rGAf0A4lk2ba2EwyJBmhDP0HNy4Ucev/uPNvzLQVVPTAhcM593LvPUHMmTYIfTi5ldW19Y38ZmFre2d3r7h/0NYyUYS2iORSdQOsKWeCtgwznHZjRXEUcNoJJleZ37mnSjMpbs00pn6ER4KFjGBjpXZfjeUFGhRLqHxer1a8KkRlhGpuxc1IpeadedC1SoYSWKI5KL73h5IkERWGcKx1z0Wx8VOsDCOczgr9RNMYkwke0Z6lAkdU++n82hk8scoQhlLZEgbO1e8TKY60nkaB7YywGevfXib+5fUSE9b9lIk4MVSQxaIw4dBImL0Oh0xRYvjUEkwUs7dCMsYKE2MDKtgQvj6F/5N2pexafuOVGpfLOPLgCByDU+CCGmiAa9AELUDAHXgAT+DZkc6j8+K8LlpzznLmEPyA8/YJcl2PCg==</latexit>

Page 14: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Dual giant: analytic continuation

⇠⇠ �X

i

y2i = �1<latexit sha1_base64="T75+gMRpB8rOBI5nXmmMpD5gIus=">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</latexit><latexit sha1_base64="T75+gMRpB8rOBI5nXmmMpD5gIus=">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</latexit><latexit sha1_base64="T75+gMRpB8rOBI5nXmmMpD5gIus=">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</latexit><latexit sha1_base64="T75+gMRpB8rOBI5nXmmMpD5gIus=">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</latexit>

✓ = 0<latexit sha1_base64="VtjVYMSbym7RPVXEZKG2onDKsuY=">AAAB73icbZA9SwNBEIbn4leMX1FLm8UgWIU7EbQRgjaWEUwMJEfY28wlS/Y+3J0TQsifsLFQxNa/Y+e/cZNcoYkvLDy8M8POvEGqpCHX/XYKK6tr6xvFzdLW9s7uXnn/oGmSTAtsiEQluhVwg0rG2CBJClupRh4FCh+C4c20/vCE2sgkvqdRin7E+7EMpeBkrVaHBkj8yu2WK27VnYktg5dDBXLVu+WvTi8RWYQxCcWNaXtuSv6Ya5JC4aTUyQymXAx5H9sWYx6h8cezfSfsxDo9FibavpjYzP09MeaRMaMosJ0Rp4FZrE3N/2rtjMJLfyzjNCOMxfyjMFOMEjY9nvWkRkFqZIELLe2uTAy45oJsRCUbgrd48jI0z6qe5bvzSu06j6MIR3AMp+DBBdTgFurQAAEKnuEV3pxH58V5dz7mrQUnnzmEP3I+fwCYO4+p</latexit><latexit sha1_base64="VtjVYMSbym7RPVXEZKG2onDKsuY=">AAAB73icbZA9SwNBEIbn4leMX1FLm8UgWIU7EbQRgjaWEUwMJEfY28wlS/Y+3J0TQsifsLFQxNa/Y+e/cZNcoYkvLDy8M8POvEGqpCHX/XYKK6tr6xvFzdLW9s7uXnn/oGmSTAtsiEQluhVwg0rG2CBJClupRh4FCh+C4c20/vCE2sgkvqdRin7E+7EMpeBkrVaHBkj8yu2WK27VnYktg5dDBXLVu+WvTi8RWYQxCcWNaXtuSv6Ya5JC4aTUyQymXAx5H9sWYx6h8cezfSfsxDo9FibavpjYzP09MeaRMaMosJ0Rp4FZrE3N/2rtjMJLfyzjNCOMxfyjMFOMEjY9nvWkRkFqZIELLe2uTAy45oJsRCUbgrd48jI0z6qe5bvzSu06j6MIR3AMp+DBBdTgFurQAAEKnuEV3pxH58V5dz7mrQUnnzmEP3I+fwCYO4+p</latexit><latexit sha1_base64="VtjVYMSbym7RPVXEZKG2onDKsuY=">AAAB73icbZA9SwNBEIbn4leMX1FLm8UgWIU7EbQRgjaWEUwMJEfY28wlS/Y+3J0TQsifsLFQxNa/Y+e/cZNcoYkvLDy8M8POvEGqpCHX/XYKK6tr6xvFzdLW9s7uXnn/oGmSTAtsiEQluhVwg0rG2CBJClupRh4FCh+C4c20/vCE2sgkvqdRin7E+7EMpeBkrVaHBkj8yu2WK27VnYktg5dDBXLVu+WvTi8RWYQxCcWNaXtuSv6Ya5JC4aTUyQymXAx5H9sWYx6h8cezfSfsxDo9FibavpjYzP09MeaRMaMosJ0Rp4FZrE3N/2rtjMJLfyzjNCOMxfyjMFOMEjY9nvWkRkFqZIELLe2uTAy45oJsRCUbgrd48jI0z6qe5bvzSu06j6MIR3AMp+DBBdTgFurQAAEKnuEV3pxH58V5dz7mrQUnnzmEP3I+fwCYO4+p</latexit><latexit sha1_base64="VtjVYMSbym7RPVXEZKG2onDKsuY=">AAAB73icbZA9SwNBEIbn4leMX1FLm8UgWIU7EbQRgjaWEUwMJEfY28wlS/Y+3J0TQsifsLFQxNa/Y+e/cZNcoYkvLDy8M8POvEGqpCHX/XYKK6tr6xvFzdLW9s7uXnn/oGmSTAtsiEQluhVwg0rG2CBJClupRh4FCh+C4c20/vCE2sgkvqdRin7E+7EMpeBkrVaHBkj8yu2WK27VnYktg5dDBXLVu+WvTi8RWYQxCcWNaXtuSv6Ya5JC4aTUyQymXAx5H9sWYx6h8cezfSfsxDo9FibavpjYzP09MeaRMaMosJ0Rp4FZrE3N/2rtjMJLfyzjNCOMxfyjMFOMEjY9nvWkRkFqZIELLe2uTAy45oJsRCUbgrd48jI0z6qe5bvzSu06j6MIR3AMp+DBBdTgFurQAAEKnuEV3pxH58V5dz7mrQUnnzmEP3I+fwCYO4+p</latexit>

Sits at “origin” in z

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Page 15: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

R-charge = Energy

E = N(1� |z|2) = N(1� cos2(✓))<latexit sha1_base64="1vxO4la17+xHCLxR9iNWtuAxabI=">AAACDHicdVDLSgMxFM34rPVVdekmWIR2YZkpim6EogiupIJ9QKctmTRtQzMPkjtCnfYD3Pgrblwo4tYPcOffmGmnoKIHAifnnEtyjxMIrsA0P425+YXFpeXUSnp1bX1jM7O1XVV+KCmrUF/4su4QxQT3WAU4CFYPJCOuI1jNGZzHfu2WScV97waGAWu6pOfxLqcEtNTOZC9O8VXOOhjdjVrFPJ5ebOqrVjFnQ58Byed1yiwcmTGwWTBnJFGsRMmiBOV25sPu+DR0mQdUEKUalhlAMyISOBVsnLZDxQJCB6THGpp6xGWqGU2WGeN9rXRw15f6eIAn6veJiLhKDV1HJ10CffXbi8W/vEYI3ZNmxL0gBObR6UPdUGDwcdwM7nDJKIihJoRKrv+KaZ9IQkH3l9YlzDbF/5NqsWBpfn2YLZ0ldaTQLtpDOWShY1RCl6iMKoiie/SIntGL8WA8Ga/G2zQ6ZyQzO+gHjPcvhVWYIg==</latexit><latexit sha1_base64="1vxO4la17+xHCLxR9iNWtuAxabI=">AAACDHicdVDLSgMxFM34rPVVdekmWIR2YZkpim6EogiupIJ9QKctmTRtQzMPkjtCnfYD3Pgrblwo4tYPcOffmGmnoKIHAifnnEtyjxMIrsA0P425+YXFpeXUSnp1bX1jM7O1XVV+KCmrUF/4su4QxQT3WAU4CFYPJCOuI1jNGZzHfu2WScV97waGAWu6pOfxLqcEtNTOZC9O8VXOOhjdjVrFPJ5ebOqrVjFnQ58Byed1yiwcmTGwWTBnJFGsRMmiBOV25sPu+DR0mQdUEKUalhlAMyISOBVsnLZDxQJCB6THGpp6xGWqGU2WGeN9rXRw15f6eIAn6veJiLhKDV1HJ10CffXbi8W/vEYI3ZNmxL0gBObR6UPdUGDwcdwM7nDJKIihJoRKrv+KaZ9IQkH3l9YlzDbF/5NqsWBpfn2YLZ0ldaTQLtpDOWShY1RCl6iMKoiie/SIntGL8WA8Ga/G2zQ6ZyQzO+gHjPcvhVWYIg==</latexit><latexit sha1_base64="1vxO4la17+xHCLxR9iNWtuAxabI=">AAACDHicdVDLSgMxFM34rPVVdekmWIR2YZkpim6EogiupIJ9QKctmTRtQzMPkjtCnfYD3Pgrblwo4tYPcOffmGmnoKIHAifnnEtyjxMIrsA0P425+YXFpeXUSnp1bX1jM7O1XVV+KCmrUF/4su4QxQT3WAU4CFYPJCOuI1jNGZzHfu2WScV97waGAWu6pOfxLqcEtNTOZC9O8VXOOhjdjVrFPJ5ebOqrVjFnQ58Byed1yiwcmTGwWTBnJFGsRMmiBOV25sPu+DR0mQdUEKUalhlAMyISOBVsnLZDxQJCB6THGpp6xGWqGU2WGeN9rXRw15f6eIAn6veJiLhKDV1HJ10CffXbi8W/vEYI3ZNmxL0gBObR6UPdUGDwcdwM7nDJKIihJoRKrv+KaZ9IQkH3l9YlzDbF/5NqsWBpfn2YLZ0ldaTQLtpDOWShY1RCl6iMKoiie/SIntGL8WA8Ga/G2zQ6ZyQzO+gHjPcvhVWYIg==</latexit><latexit sha1_base64="1vxO4la17+xHCLxR9iNWtuAxabI=">AAACDHicdVDLSgMxFM34rPVVdekmWIR2YZkpim6EogiupIJ9QKctmTRtQzMPkjtCnfYD3Pgrblwo4tYPcOffmGmnoKIHAifnnEtyjxMIrsA0P425+YXFpeXUSnp1bX1jM7O1XVV+KCmrUF/4su4QxQT3WAU4CFYPJCOuI1jNGZzHfu2WScV97waGAWu6pOfxLqcEtNTOZC9O8VXOOhjdjVrFPJ5ebOqrVjFnQ58Byed1yiwcmTGwWTBnJFGsRMmiBOV25sPu+DR0mQdUEKUalhlAMyISOBVsnLZDxQJCB6THGpp6xGWqGU2WGeN9rXRw15f6eIAn6veJiLhKDV1HJ10CffXbi8W/vEYI3ZNmxL0gBObR6UPdUGDwcdwM7nDJKIihJoRKrv+KaZ9IQkH3l9YlzDbF/5NqsWBpfn2YLZ0ldaTQLtpDOWShY1RCl6iMKoiie/SIntGL8WA8Ga/G2zQ6ZyQzO+gHjPcvhVWYIg==</latexit>

For giants:

For dual giants:

E = N(|⇠|2 � 1) = N(cosh2(⇢)� 1)<latexit sha1_base64="HRU5xhSCAJINAWy9L9m2JDMIQX8=">AAACDXicdZDLSgMxFIYz9VbrbdSlm2AV2oVlpii6EYoiuJIK9gKdtmTStBOamQxJRixtX8CNr+LGhSJu3bvzbcy0U1DRHwJ/vnMOyfndkFGpLOvTSM3NLywupZczK6tr6xvm5lZV8khgUsGccVF3kSSMBqSiqGKkHgqCfJeRmts/j+u1WyIk5cGNGoSk6aNeQLsUI6VR29y7OIVXuZFzR0et4oGdh/HVwVx6rWLOER7Pa9g2s1bhyIoFrYI1MwmxE5IFicpt88PpcBz5JFCYISkbthWq5hAJRTEj44wTSRIi3Ec90tA2QD6RzeFkmzHc16QDu1zoEyg4od8nhsiXcuC7utNHypO/azH8q9aIVPekOaRBGCkS4OlD3YhBxWEcDexQQbBiA20QFlT/FWIPCYSVDjCjQ5htCv831WLB1v76MFs6S+JIgx2wC3LABsegBC5BGVQABvfgETyDF+PBeDJejbdpa8pIZrbBDxnvX07jmIo=</latexit><latexit sha1_base64="HRU5xhSCAJINAWy9L9m2JDMIQX8=">AAACDXicdZDLSgMxFIYz9VbrbdSlm2AV2oVlpii6EYoiuJIK9gKdtmTStBOamQxJRixtX8CNr+LGhSJu3bvzbcy0U1DRHwJ/vnMOyfndkFGpLOvTSM3NLywupZczK6tr6xvm5lZV8khgUsGccVF3kSSMBqSiqGKkHgqCfJeRmts/j+u1WyIk5cGNGoSk6aNeQLsUI6VR29y7OIVXuZFzR0et4oGdh/HVwVx6rWLOER7Pa9g2s1bhyIoFrYI1MwmxE5IFicpt88PpcBz5JFCYISkbthWq5hAJRTEj44wTSRIi3Ec90tA2QD6RzeFkmzHc16QDu1zoEyg4od8nhsiXcuC7utNHypO/azH8q9aIVPekOaRBGCkS4OlD3YhBxWEcDexQQbBiA20QFlT/FWIPCYSVDjCjQ5htCv831WLB1v76MFs6S+JIgx2wC3LABsegBC5BGVQABvfgETyDF+PBeDJejbdpa8pIZrbBDxnvX07jmIo=</latexit><latexit sha1_base64="HRU5xhSCAJINAWy9L9m2JDMIQX8=">AAACDXicdZDLSgMxFIYz9VbrbdSlm2AV2oVlpii6EYoiuJIK9gKdtmTStBOamQxJRixtX8CNr+LGhSJu3bvzbcy0U1DRHwJ/vnMOyfndkFGpLOvTSM3NLywupZczK6tr6xvm5lZV8khgUsGccVF3kSSMBqSiqGKkHgqCfJeRmts/j+u1WyIk5cGNGoSk6aNeQLsUI6VR29y7OIVXuZFzR0et4oGdh/HVwVx6rWLOER7Pa9g2s1bhyIoFrYI1MwmxE5IFicpt88PpcBz5JFCYISkbthWq5hAJRTEj44wTSRIi3Ec90tA2QD6RzeFkmzHc16QDu1zoEyg4od8nhsiXcuC7utNHypO/azH8q9aIVPekOaRBGCkS4OlD3YhBxWEcDexQQbBiA20QFlT/FWIPCYSVDjCjQ5htCv831WLB1v76MFs6S+JIgx2wC3LABsegBC5BGVQABvfgETyDF+PBeDJejbdpa8pIZrbBDxnvX07jmIo=</latexit><latexit sha1_base64="HRU5xhSCAJINAWy9L9m2JDMIQX8=">AAACDXicdZDLSgMxFIYz9VbrbdSlm2AV2oVlpii6EYoiuJIK9gKdtmTStBOamQxJRixtX8CNr+LGhSJu3bvzbcy0U1DRHwJ/vnMOyfndkFGpLOvTSM3NLywupZczK6tr6xvm5lZV8khgUsGccVF3kSSMBqSiqGKkHgqCfJeRmts/j+u1WyIk5cGNGoSk6aNeQLsUI6VR29y7OIVXuZFzR0et4oGdh/HVwVx6rWLOER7Pa9g2s1bhyIoFrYI1MwmxE5IFicpt88PpcBz5JFCYISkbthWq5hAJRTEj44wTSRIi3Ec90tA2QD6RzeFkmzHc16QDu1zoEyg4od8nhsiXcuC7utNHypO/azH8q9aIVPekOaRBGCkS4OlD3YhBxWEcDexQQbBiA20QFlT/FWIPCYSVDjCjQ5htCv831WLB1v76MFs6S+JIgx2wC3LABsegBC5BGVQABvfgETyDF+PBeDJejbdpa8pIZrbBDxnvX07jmIo=</latexit>

Page 16: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Energies up to

O(N)<latexit sha1_base64="pHGyu6r4U0O4KCziVrGUXTuKBqc=">AAAB7HicdVBdSwJBFL1rX2ZfVo+9DElgL7Jri9qb1EtPZdCqoCKz46wOzs4uM7OBiL+hlx6K6LUf1Fv/plk1qKgDFw7n3Mu99/gxZ0rb9oeVWVldW9/Ibua2tnd29/L7B00VJZJQj0Q8km0fK8qZoJ5mmtN2LCkOfU5b/vgy9Vv3VCoWiTs9iWkvxEPBAkawNpJ3U0TXp/18wS6d1yplt4Lskm1XnbKTknLVPXORY5QUBVii0c+/dwcRSUIqNOFYqY5jx7o3xVIzwuks100UjTEZ4yHtGCpwSFVvOj92hk6MMkBBJE0Jjebq94kpDpWahL7pDLEeqd9eKv7ldRId1HpTJuJEU0EWi4KEIx2h9HM0YJISzSeGYCKZuRWREZaYaJNPzoTw9Sn6nzTLJcfwW7dQv1jGkYUjOIYiOFCFOlxBAzwgwOABnuDZEtaj9WK9Lloz1nLmEH7AevsEv56N/A==</latexit><latexit sha1_base64="pHGyu6r4U0O4KCziVrGUXTuKBqc=">AAAB7HicdVBdSwJBFL1rX2ZfVo+9DElgL7Jri9qb1EtPZdCqoCKz46wOzs4uM7OBiL+hlx6K6LUf1Fv/plk1qKgDFw7n3Mu99/gxZ0rb9oeVWVldW9/Ibua2tnd29/L7B00VJZJQj0Q8km0fK8qZoJ5mmtN2LCkOfU5b/vgy9Vv3VCoWiTs9iWkvxEPBAkawNpJ3U0TXp/18wS6d1yplt4Lskm1XnbKTknLVPXORY5QUBVii0c+/dwcRSUIqNOFYqY5jx7o3xVIzwuks100UjTEZ4yHtGCpwSFVvOj92hk6MMkBBJE0Jjebq94kpDpWahL7pDLEeqd9eKv7ldRId1HpTJuJEU0EWi4KEIx2h9HM0YJISzSeGYCKZuRWREZaYaJNPzoTw9Sn6nzTLJcfwW7dQv1jGkYUjOIYiOFCFOlxBAzwgwOABnuDZEtaj9WK9Lloz1nLmEH7AevsEv56N/A==</latexit><latexit sha1_base64="pHGyu6r4U0O4KCziVrGUXTuKBqc=">AAAB7HicdVBdSwJBFL1rX2ZfVo+9DElgL7Jri9qb1EtPZdCqoCKz46wOzs4uM7OBiL+hlx6K6LUf1Fv/plk1qKgDFw7n3Mu99/gxZ0rb9oeVWVldW9/Ibua2tnd29/L7B00VJZJQj0Q8km0fK8qZoJ5mmtN2LCkOfU5b/vgy9Vv3VCoWiTs9iWkvxEPBAkawNpJ3U0TXp/18wS6d1yplt4Lskm1XnbKTknLVPXORY5QUBVii0c+/dwcRSUIqNOFYqY5jx7o3xVIzwuks100UjTEZ4yHtGCpwSFVvOj92hk6MMkBBJE0Jjebq94kpDpWahL7pDLEeqd9eKv7ldRId1HpTJuJEU0EWi4KEIx2h9HM0YJISzSeGYCKZuRWREZaYaJNPzoTw9Sn6nzTLJcfwW7dQv1jGkYUjOIYiOFCFOlxBAzwgwOABnuDZEtaj9WK9Lloz1nLmEH7AevsEv56N/A==</latexit><latexit sha1_base64="pHGyu6r4U0O4KCziVrGUXTuKBqc=">AAAB7HicdVBdSwJBFL1rX2ZfVo+9DElgL7Jri9qb1EtPZdCqoCKz46wOzs4uM7OBiL+hlx6K6LUf1Fv/plk1qKgDFw7n3Mu99/gxZ0rb9oeVWVldW9/Ibua2tnd29/L7B00VJZJQj0Q8km0fK8qZoJ5mmtN2LCkOfU5b/vgy9Vv3VCoWiTs9iWkvxEPBAkawNpJ3U0TXp/18wS6d1yplt4Lskm1XnbKTknLVPXORY5QUBVii0c+/dwcRSUIqNOFYqY5jx7o3xVIzwuks100UjTEZ4yHtGCpwSFVvOj92hk6MMkBBJE0Jjebq94kpDpWahL7pDLEeqd9eKv7ldRId1HpTJuJEU0EWi4KEIx2h9HM0YJISzSeGYCKZuRWREZaYaJNPzoTw9Sn6nzTLJcfwW7dQv1jGkYUjOIYiOFCFOlxBAzwgwOABnuDZEtaj9WK9Lloz1nLmEH7AevsEv56N/A==</latexit>

Page 17: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Multi-traces, although BPS, are not orthogonal at finite N.

Need another orthogonal basis to describe finite N physics.

Page 18: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

How do these fit? Dual operators

Page 19: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

To build gauge invariants, need to contract upper and lower indices in Z

Zi1i01. . . Zik

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Free theory has a symmetry of upper and lower indices

SU(N)U ⇥ SU(N)D<latexit sha1_base64="fk5FTS1iEWuqImgjfRog3vWhpkQ=">AAAB/nicdVDLSsNAFL3xWesrKq7cDBahbkoiii6LunAlFU1baEOYTCft0MmDmYlQQsFfceNCEbd+hzv/xkmbgooeGDj3nHu5d46fcCaVZX0ac/MLi0vLpZXy6tr6xqa5td2UcSoIdUjMY9H2saScRdRRTHHaTgTFoc9pyx9e5H7rngrJ4uhOjRLqhrgfsYARrLTkmbu3TvX60HO6ioVUoml16ZkVq3Zi5UBWzZqRQrELpQIFGp750e3FJA1ppAjHUnZsK1FuhoVihNNxuZtKmmAyxH3a0TTCepmbTc4fowOt9FAQC/0ihSbq94kMh1KOQl93hlgN5G8vF//yOqkKztyMRUmqaESmi4KUIxWjPAvUY4ISxUeaYCKYvhWRARaYKJ1YWYcw+yn6nzSParbmN8eV+nkRRwn2YB+qYMMp1OEKGuAAgQwe4RlejAfjyXg13qatc0YxswM/YLx/AbxDlAo=</latexit><latexit sha1_base64="fk5FTS1iEWuqImgjfRog3vWhpkQ=">AAAB/nicdVDLSsNAFL3xWesrKq7cDBahbkoiii6LunAlFU1baEOYTCft0MmDmYlQQsFfceNCEbd+hzv/xkmbgooeGDj3nHu5d46fcCaVZX0ac/MLi0vLpZXy6tr6xqa5td2UcSoIdUjMY9H2saScRdRRTHHaTgTFoc9pyx9e5H7rngrJ4uhOjRLqhrgfsYARrLTkmbu3TvX60HO6ioVUoml16ZkVq3Zi5UBWzZqRQrELpQIFGp750e3FJA1ppAjHUnZsK1FuhoVihNNxuZtKmmAyxH3a0TTCepmbTc4fowOt9FAQC/0ihSbq94kMh1KOQl93hlgN5G8vF//yOqkKztyMRUmqaESmi4KUIxWjPAvUY4ISxUeaYCKYvhWRARaYKJ1YWYcw+yn6nzSParbmN8eV+nkRRwn2YB+qYMMp1OEKGuAAgQwe4RlejAfjyXg13qatc0YxswM/YLx/AbxDlAo=</latexit><latexit sha1_base64="fk5FTS1iEWuqImgjfRog3vWhpkQ=">AAAB/nicdVDLSsNAFL3xWesrKq7cDBahbkoiii6LunAlFU1baEOYTCft0MmDmYlQQsFfceNCEbd+hzv/xkmbgooeGDj3nHu5d46fcCaVZX0ac/MLi0vLpZXy6tr6xqa5td2UcSoIdUjMY9H2saScRdRRTHHaTgTFoc9pyx9e5H7rngrJ4uhOjRLqhrgfsYARrLTkmbu3TvX60HO6ioVUoml16ZkVq3Zi5UBWzZqRQrELpQIFGp750e3FJA1ppAjHUnZsK1FuhoVihNNxuZtKmmAyxH3a0TTCepmbTc4fowOt9FAQC/0ihSbq94kMh1KOQl93hlgN5G8vF//yOqkKztyMRUmqaESmi4KUIxWjPAvUY4ISxUeaYCKYvhWRARaYKJ1YWYcw+yn6nzSParbmN8eV+nkRRwn2YB+qYMMp1OEKGuAAgQwe4RlejAfjyXg13qatc0YxswM/YLx/AbxDlAo=</latexit><latexit sha1_base64="fk5FTS1iEWuqImgjfRog3vWhpkQ=">AAAB/nicdVDLSsNAFL3xWesrKq7cDBahbkoiii6LunAlFU1baEOYTCft0MmDmYlQQsFfceNCEbd+hzv/xkmbgooeGDj3nHu5d46fcCaVZX0ac/MLi0vLpZXy6tr6xqa5td2UcSoIdUjMY9H2saScRdRRTHHaTgTFoc9pyx9e5H7rngrJ4uhOjRLqhrgfsYARrLTkmbu3TvX60HO6ioVUoml16ZkVq3Zi5UBWzZqRQrELpQIFGp750e3FJA1ppAjHUnZsK1FuhoVihNNxuZtKmmAyxH3a0TTCepmbTc4fowOt9FAQC/0ihSbq94kMh1KOQl93hlgN5G8vF//yOqkKztyMRUmqaESmi4KUIxWjPAvUY4ISxUeaYCKYvhWRARaYKJ1YWYcw+yn6nzSParbmN8eV+nkRRwn2YB+qYMMp1OEKGuAAgQwe4RlejAfjyXg13qatc0YxswM/YLx/AbxDlAo=</latexit>

where a particular diagonal embedding is gauged.

Page 20: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Decompose tensor into irreps of this extra symmetry:Young diagram for upper and lower indices.

This is the Schur polynomial basis.

Unique gauge invariant built from this data.

Corley, Jevicki, Ramgoolam hep-th/0111222

Page 21: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

How they match

• Giants are sub-determinants (1-column)

• Balasubramanian, Berkooz, Naqvi, Strassler hep-th/0107119

• Dual giants are 1-row.

• CJR

Page 22: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

These are D-branes, so strings must end on them (somehow).

Berenstein, Balasubramanian, Feng, Huang, hep-th/0411205

Idea: intertwine indices of extra letters with the Z in a column or rowto produce open strings spin chains with interesting boundary conditions.

Page 23: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Many years of work by various groups

R. de Mello Koch et al; S. Ramgoolam et al; (constructing restricted Schur basis

and learning how to count states and compute)

Berenstein et al. (understanding boundary conditions on spin chains+collective coordinates+solving for ground state)

Page 24: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

What does it look like?

Page 25: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small
Page 26: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

When considering bigger sectors with SUSY,

{Q,Q} / exp(ip)

one can associate a central charge to the spin chain (Beisert).

Y ! [Y, Z]

Which shows effectively as follows

Evaluating one gets

This is evaluated on a single magnon.

Page 27: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Produces a non-trivial dispersion relation for impurity

�� J 'q

1 + h(�) sin2 p/2

Good to “all orders”h(�) = �

This is the strong ’t Hooft coupling constant.

Page 28: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

This is the dispersion relation of a giant magnon: a piece of string

that is a straight chord between two end-points on a disk, moving with angular velocity one

S3 ! S5

#D2

(Hofmann -Maldacena)

Same coordinates as before

See also talk by Jaco van Zyl.

Page 29: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

D.B., E. Dziekowski arXiv:1408.3620

Page 30: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

The D-branes have sourced the central charge of Beisert.

Page 31: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Bubbling geometries

Page 32: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Can one solve the most general half BPS state in

gravity?

Page 33: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Matrix model ideas suggest that the Schurs are well described by free fermions.

Ideal representation is by using a holomorphic representation of this structure: free fermions in phase space (same physics as Quantum Hall

droplets)

DB, hep-th/0403110

In this representation traces are single quanta of edge states, whereas dual giants and giants are fermions (eigenvalues) and holes removed from the droplet

respectively

Page 34: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Suggests that the most general “classical limit” is of incompressible droplets in a 2D plane.

This is realized exactly in gravity!

Page 35: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

LLM geometries

ds2 = � yq14 � z2

(dt+ Vidxi)2 +

q14 � z2

y(dy2 + dxidxi)

+y

s12 � z12 + z

!d⌦2

3 + y

s12 + z12 � z

!d⌦2

3

Lin, Lunin, Maldacena, JHEP 0410 (2004) 025

Solutions of type IIB supergravity, that preserve half the SUSY

+ attendant fluxes

Page 36: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

depend on a single function z(~x, y)

@i@iz + y@y

✓@yz

y

◆= 0

Satisfies an ordinary linear PDE

Reality of the metric requires that

|z| 1

2

Page 37: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Degeneration at y=0

This provides a two coloring of the plane.

These are all horizon free smooth 10 D geometries.

Absence of conical singularity forces

z(0, ~x) = ±1

2

Page 38: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

A typical LLM geometry

Topology of picture encodes topology of spacetime: different picture topologies give rise to different spacetime

topologies.

Have conserved area and an energy function.

Page 39: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

N =

Z⇢(~x)d2x

They have a conserved “flux”

An energy function

Area of the droplet

E =

Z⇢(~x)~x2d2x� E�

Page 40: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Complete classification

Page 41: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Has energies of order

O(N2)<latexit sha1_base64="LmlaKfhQyGSZDBv5Fqvma5WdWf8=">AAAB7nicdVDLSgNBEOz1GeMr6tHLYBDiJeyuSxJvQS+eNIJ5QLKG2clsMmT2wcysEJZ8hBcPinj1e7z5N84mEVS0oKGo6qa7y4s5k8o0P4yl5ZXVtfXcRn5za3tnt7C335JRIghtkohHouNhSTkLaVMxxWknFhQHHqdtb3yR+e17KiSLwls1iakb4GHIfEaw0lL7uoSu7uyTfqFols9qFdupILNsmlXLtjJiV51TB1layVCEBRr9wntvEJEkoKEiHEvZtcxYuSkWihFOp/leImmMyRgPaVfTEAdUuuns3Ck61soA+ZHQFSo0U79PpDiQchJ4ujPAaiR/e5n4l9dNlF9zUxbGiaIhmS/yE45UhLLf0YAJShSfaIKJYPpWREZYYKJ0Qnkdwten6H/SssuW5jdOsX6+iCMHh3AEJbCgCnW4hAY0gcAYHuAJno3YeDRejNd565KxmDmAHzDePgHmf46g</latexit><latexit sha1_base64="LmlaKfhQyGSZDBv5Fqvma5WdWf8=">AAAB7nicdVDLSgNBEOz1GeMr6tHLYBDiJeyuSxJvQS+eNIJ5QLKG2clsMmT2wcysEJZ8hBcPinj1e7z5N84mEVS0oKGo6qa7y4s5k8o0P4yl5ZXVtfXcRn5za3tnt7C335JRIghtkohHouNhSTkLaVMxxWknFhQHHqdtb3yR+e17KiSLwls1iakb4GHIfEaw0lL7uoSu7uyTfqFols9qFdupILNsmlXLtjJiV51TB1layVCEBRr9wntvEJEkoKEiHEvZtcxYuSkWihFOp/leImmMyRgPaVfTEAdUuuns3Ck61soA+ZHQFSo0U79PpDiQchJ4ujPAaiR/e5n4l9dNlF9zUxbGiaIhmS/yE45UhLLf0YAJShSfaIKJYPpWREZYYKJ0Qnkdwten6H/SssuW5jdOsX6+iCMHh3AEJbCgCnW4hAY0gcAYHuAJno3YeDRejNd565KxmDmAHzDePgHmf46g</latexit><latexit sha1_base64="LmlaKfhQyGSZDBv5Fqvma5WdWf8=">AAAB7nicdVDLSgNBEOz1GeMr6tHLYBDiJeyuSxJvQS+eNIJ5QLKG2clsMmT2wcysEJZ8hBcPinj1e7z5N84mEVS0oKGo6qa7y4s5k8o0P4yl5ZXVtfXcRn5za3tnt7C335JRIghtkohHouNhSTkLaVMxxWknFhQHHqdtb3yR+e17KiSLwls1iakb4GHIfEaw0lL7uoSu7uyTfqFols9qFdupILNsmlXLtjJiV51TB1layVCEBRr9wntvEJEkoKEiHEvZtcxYuSkWihFOp/leImmMyRgPaVfTEAdUuuns3Ck61soA+ZHQFSo0U79PpDiQchJ4ujPAaiR/e5n4l9dNlF9zUxbGiaIhmS/yE45UhLLf0YAJShSfaIKJYPpWREZYYKJ0Qnkdwten6H/SssuW5jdOsX6+iCMHh3AEJbCgCnW4hAY0gcAYHuAJno3YeDRejNd565KxmDmAHzDePgHmf46g</latexit><latexit sha1_base64="LmlaKfhQyGSZDBv5Fqvma5WdWf8=">AAAB7nicdVDLSgNBEOz1GeMr6tHLYBDiJeyuSxJvQS+eNIJ5QLKG2clsMmT2wcysEJZ8hBcPinj1e7z5N84mEVS0oKGo6qa7y4s5k8o0P4yl5ZXVtfXcRn5za3tnt7C335JRIghtkohHouNhSTkLaVMxxWknFhQHHqdtb3yR+e17KiSLwls1iakb4GHIfEaw0lL7uoSu7uyTfqFols9qFdupILNsmlXLtjJiV51TB1layVCEBRr9wntvEJEkoKEiHEvZtcxYuSkWihFOp/leImmMyRgPaVfTEAdUuuns3Ck61soA+ZHQFSo0U79PpDiQchJ4ujPAaiR/e5n4l9dNlF9zUxbGiaIhmS/yE45UhLLf0YAJShSfaIKJYPpWREZYYKJ0Qnkdwten6H/SssuW5jdOsX6+iCMHh3AEJbCgCnW4hAY0gcAYHuAJno3YeDRejNd565KxmDmAHzDePgHmf46g</latexit>

Page 42: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Beyond

• Same energies, but not BPS= black hole physics

• Thermal field theory at high T

• Much less is known

• Specific heat of free field theory is of the correct order if magnitude to compare to specific heat of black hole

Page 43: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Other results

• Wilson loops and localization (different kind of matrix models)

• Helicity methods (integrability in S-matrix)

• Other CFT’s: ABJM, SUSY flows

• HKLL bulk reconstruction methods.

Page 44: Aspects of the AdS/ CFT dictionary, IIneo.phys.wits.ac.za/workshop_12/David2.pdfWe want to explore CFT at large values of R -large ‘t Hooft coupling- but with g fixed and small

Conclusion

• We know a lot of pieces of the dictionary

• Still a lot to learn

• Black holes and horizon dynamics are still a mystery.