O ( d , d ) preserve classical integrability Yuta Sekiguchi - - PowerPoint PPT Presentation

o d d
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O ( d , d ) preserve classical integrability Yuta Sekiguchi - - PowerPoint PPT Presentation

transformations O ( d , d ) preserve classical integrability Yuta Sekiguchi University of Bern (AEC, ITP) Strings and Fields 2019 @ YITP, Kyoto Based on 1907.03759 with Domenico Orlando (INFN, Turin), Susanne Reffert (University of


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SLIDE 1
  • transformations

preserve classical integrability

O(d, d)

Strings and Fields 2019 @ YITP, Kyoto Based on 1907.03759 with Kentaroh Yoshida (Kyoto University) Domenico Orlando (INFN, Turin), Susanne Reffert (University of Bern), and

Yuta Sekiguchi

University of Bern (AEC, ITP) cf: [Ricci, Tseytlin, Wolf 2007], [Rennecke 2014], and [Hull 2004]
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SLIDE 2
  • 1. Motivation
  • 2. Classical integrability of WZW models
  • 3. Doubled formalism and

transf.

  • 4. Application
  • 5. Outlook

O(d, d)

The plan of my talk

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SLIDE 3
  • 1. Motivation

(Quick!)

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SLIDE 4

1.2 Classical integrability of string theory

4
  • AdSd/CFTd-1: attractive examples of Gauge/Gravity duality
d=5: [Maldacena-1998] type IIB string on AdS5xS5 4D N=4 SU(N) SYM (N→∞) ‘ ’
  • Intriguing: integrable structures
allows us to determine physical quantities exactly, even at finite coupling, without relying on supersymmetries. A comprehensive review: [Beisert et al-2010] e.g. scattering amplitudes, conformal dims. of composite ops. spectrum of strings etc… → Many directions of applications of integrability techniques! An ongoing series of winter schools
  • f integrability (=YRISW)
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SLIDE 5
  • AdSd/CFTd-1: attractive examples of Gauge/Gravity duality
d=5: type IIB string on AdS5xS5 4D N≦4 SU(N) SYM (N→∞) ‘ ’ deformed deformed integrable integrable e.g. scattering amplitudes, conformal dims. of composite ops. spectrum of strings etc…
  • Significant: integrable deformations
construct a variety of examples of ↑dualities keeping the integrability

1.2 Classical integrability of string theory

  • Intriguing: integrable structures
allows us to determine physical quantities exactly, even at finite coupling, without relying on supersymmetries. → Want to follow a systematic approach for such deformations. → Yang-Baxter deformation 5
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SLIDE 6 \

1.3 A bit about Yang-Baxter deformation

  • The YB deformed σ-model action (w/ WZ-term: )
[Klimcik 02, 08] Sλ = Z d2σ ηab Tr  Ja 1 1 − λ RJb
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↑ const. deformation parameter
  • A linear operator R : g → g
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  • The classical r-matrix is a solution of classical YB equation (CYBE)
[r12, r13] + [r12, r23] + [r13, r23] = 0 <latexit sha1_base64="IAUkEHKVG9zvlTGi6Una1flBDEw=">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</latexit><latexit 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slide-7
SLIDE 7 \

1.3 Yang-Baxter (YB) deformation

In summary, the method consists of
  • 1. Put classical r-matrix into the YB deformed sigma model action:
  • const. deformation parameter↑
  • 2. Rewrite the action to read off the deformed background data
by comparing with the canonical formula: S = − √c 4 Z ∞ −∞ d⌧ Z 2π d  abGMN@aXM@bXN − ✏abBMN@aXM@bXN
√c 2 i¯ ΘI ⇥ abIJ − ✏abIJ 3 ⇤ em a ΓmDJK b ΘK + O(✓4) <latexit sha1_base64="lykUs3dEBMl5g14uLF48Yjld+4Y=">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</latexit><latexit sha1_base64="lykUs3dEBMl5g14uLF48Yjld+4Y=">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</latexit><latexit sha1_base64="lykUs3dEBMl5g14uLF48Yjld+4Y=">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</latexit><latexit sha1_base64="qRC7+D4EgJpw9EXVPOLCYWDAD3E=">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</latexit> with DIJ a = IJ(@a − 1 4!mn a Γmn) + 1 8IJ 3 em a HmnpΓnp − eΦ 8  ✏IJΓpFp + 1 3!IJ 1 ΓpqrFpar + 1 2 · 5!✏IJΓpqrstFpqrst
  • em
a Γm <latexit sha1_base64="4bLtmrC+z5Nh/PNeM6/jb4NY40=">AETXiclVHLbtNAFL1xCi3h0RQ2SGwMEVRaTRuiygLpEgKIhFEKStlEmisTNxRvWr4wlSZeYH+BIQP8KOFQs+gAVrhNhUiOvJi7ZQ6Fi275w59zHuEkgUkXI54JVnDlzdnbuXOn8hYuX5sLl7fSeCA93vDiIJY7Lkt5ICLeUEIFfCeRnIVuwLfd3Qf5+fYrLlMRy/VfsJbIfMj0RMeUwh1FgpfHrazJ091J2PaXrxv0y4PFDPQEk2YVIF5mzFpj3JvMzR2bqmch9luPtLIw0fczCELcY3rKXp8QNTVPh2yUYU1zpJtUmzk5GQnbWR7S0uLKUJlR01dT+m4rc6rErNvkaJC70XpfaG0yucL3gyblSqCODIpx/aJ/l/LRx0k6+VJB2vXD7fgTD35Klcmfzd5V63VjdQfc/1rsnU3UqdyMYzkC2JlOe3IvulCtjvn08GJtXajaYVY/Lb4FCF2LwYAhcIhAYRwAgxSfJjhAIEGsBRliEiNhzjloKF2gCyODIboLn593DVHaIT73DM1ag+zBPhKVNpwk3wi78g38oG8J1/JwV+9MuOR17KPf3eo5Uln/s3VFz/+qQrxr6A/VZ1Ys4IebJhaBdaeGCTvwjuh1wyx4bT6uOtCfgXO0YEfD7ZWqw6pOs/XK7V7w7uAObgGN2AJ34XarAJdWiAZz2zpJVZr4sfi9+LB8WfQ6pVGmuwKE1M/sL0BAu/A=</latexit><latexit sha1_base64="4bLtmrC+z5Nh/PNeM6/jb4NY40=">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</latexit><latexit sha1_base64="4bLtmrC+z5Nh/PNeM6/jb4NY40=">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</latexit><latexit sha1_base64="dUD4XkzF84NzRBCD8TtZHxjCyaw=">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</latexit> S = pc 4 Z ∞ −∞ d⌧ Z 2π d(ab ✏ab)STr  Ja d 1 1 R d(Jb)
  • <latexit sha1_base64="GwNgsSe4Jvn50hwsXDSVIvnzft4=">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</latexit><latexit sha1_base64="GwNgsSe4Jvn50hwsXDSVIvnzft4=">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</latexit><latexit sha1_base64="GwNgsSe4Jvn50hwsXDSVIvnzft4=">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</latexit><latexit sha1_base64="Lnmkr2r0PhNzClrxwH1aszrQ5eE=">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</latexit>
[Cvetic-Lu-Pope-Stelle]
  • cl. r-matrix inserted.
[Delduc, Magro, Vicedo], [Matsumoto, Yoshida] [Kawaguchi, Matsumoto, Yoshida] 7
slide-8
SLIDE 8 \

1.3 Yang-Baxter (YB) deformation

Important observations: Yang-Baxter → O(d, d) Some YB-deformations related to transformations (or T-duality) O(d, d) ☆ TsT (T-duality-shift-T-duality) transformation on T2 ☆ T-fold (non-geometric) backgrounds ~ some local O(d, d) ☆ Some current-current deformations ~ some global O(d, d) ☆ Non-abelian T-dual backgrounds Complimentary: focus on integrability of without Yang-Baxter O(d, d; ℝ) → Use the
  • invariant formalism
O(d, d) → To understand classical integrability of non-geometric backgrounds, started to focus on global transformations O(d, d; ℝ) T-duality vs. conformal symmetry on (dual conformal symmetry), AdS5 × S5
  • deformation (see Kentaroh’s talk)
T ¯ T Other motivations: [Alday, Aturyunov, Frolov] etc… [Borsato, Wulff] [Araujo et al] [Fernandez-Melgarejo et al] [Borsato, Wulff] [Ricci, Tseytlin, Wolf], [Beisert] [Giveon, Itzhaki, Kutasov] etc… [Hull] 8
slide-9
SLIDE 9

1.4 Upshot

☆ Motivated by two recent developments in string theory
  • 1. Classical integrability of string theory
  • 2. Duality invariant approach to string theory

}

☆ Take home message: a synthetic study of the above topics
  • Systematically obtained
  • deformed Lax pairs

O(d, d)

via doubled formalism (or
  • map)

O(d, d)

  • Global
transformations = integrable

O(d, d; ℝ)

9
slide-10
SLIDE 10

WZW

  • 2. Classical integrability

(=the existence of Lax pairs)

  • f WZW models
slide-11
SLIDE 11

2.1 Basics of WZW model (on w/ -flux)

S3 H

\ Given the action S[g] = −1 4 Z Σ2 Tr [jL ∧ ?jL] + i 3! Z V3 Tr [jL ∧ jL ∧ jL] <latexit sha1_base64="aLE3Dbq+3tIaISejnHl3Bc30p3o=">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</latexit> (Six) Noether currents (for ): SU(2)L × SU(2)R JL = (1 − i ?) jL , JR = (1 + i ?) jR <latexit sha1_base64="ZzjmKj+8hF5b17TqEIn48YlqVU=">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</latexit> (and flat) jL = +g−1dg jR = −dg g−1 <latexit sha1_base64="S4wt6pxlLGXB4b70z3Z1yEcVtJg=">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</latexit> → (Six) Lax pairs given by aλ = 1 2 (1 − cosh λ) bλ = 1 2 sinh λ <latexit sha1_base64="ZhBuODgtR+XpT969dDgnPqVqREg=">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</latexit> LL/R = aλJL/R + bλ ? JL/R <latexit sha1_base64="2PxY464y9Wrvfr4VHjSVU9zfF8=">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</latexit> dL + L ∧ L = 0 <latexit sha1_base64="VEr079Rtd3X6kY5xUKIbjEfWY=">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</latexit> satisfying on-shell for and . L R (flatness, zero-curvature condition) : spectral parameter λ 11
slide-12
SLIDE 12

2.2 Lax pair and monodromy matrix

\ Given Lax pairs, the monodromy matrix satisfying the conservation laws: T (τ; λ) = Pexp  − Z +1 1 dσ0Lσ(σ0)
  • = 1 +
1 X n=0 λn+1Q(n)(τ) <latexit sha1_base64="j3I48Af4RiEfTuDJcGUaVTmO5c=">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</latexit> ∂ ∂τ Q(n) = 0, n ∈ Z≥0 <latexit sha1_base64="p8n1O84CB4XJpzXLyA7+1s+bBFI=">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</latexit> The -number of conserved charges written in non-local forms. Intriguing: determine the type of algebra for their commutators. (using flatness of Lax pairs) Note: Lax connections (flat currents) are unique up to gauge transf.

L → ˆ L = h−1L h + h−1dh

<latexit sha1_base64="ouRJea8AayO9FtdDqzUZ1tfngZA=">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</latexit> h ∈ G <latexit sha1_base64="LeD6bqJf0L+v1n65QMTjzdmy0=">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</latexit> 12
slide-13
SLIDE 13

2.3 Concrete gauged Lax pairs for w/ -flux

S3 H

\ Given an element SU(2) g = e−Z+T2eY T1e+Z−T2 = e−(Z1+Z2)T2eY T1e+(Z1−Z2)T2 <latexit sha1_base64="eUE7Cn0PezC5s752fytRmQz5fs4=">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</latexit> [Tα, Tβ] = ✏αβγTγ, Tr (TαTβ) = −1 2αβ, ✏123 = 1 <latexit sha1_base64="dcj8AnyecY8fozarmbkpbshd1w=">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</latexit> and , the gauged Lax pairs are

}

hL = e−(Z1−Z2)T2 hR = e−(Z1+Z2)T2 <latexit sha1_base64="8X4oSAI6sH/bR0Mz6Tlp/D+ElE=">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</latexit> for L for R 13
slide-14
SLIDE 14

2.3 Concrete gauged Lax pairs for w/ -flux

S3 H

\ Given an element SU(2) g = e−Z+T2eY T1e+Z−T2 = e−(Z1+Z2)T2eY T1e+(Z1−Z2)T2 <latexit sha1_base64="eUE7Cn0PezC5s752fytRmQz5fs4=">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</latexit> [Tα, Tβ] = ✏αβγTγ, Tr (TαTβ) = −1 2αβ, ✏123 = 1 <latexit sha1_base64="dcj8AnyecY8fozarmbkpbshd1w=">AEQHichVJNaxNBGH6360etH0VRPCyGCIVaphNBUqFkXx0EObJm0hG8LsZpJdOvh7CQSl/0D/gEPnhQ8iBd/g178Ax76DxQPKhUE8eC7s7Ghtkln2J1n3vd5nw464F0tCdrQp/djxEyenT82cPnP23Gxh7vxGHPaEw+pOyEOxZdOYcS9gdelJzrYiwahvc7Zpb9/P8pt9JmIvDGpyELGmT7uB1/EcKjHUKrxr1FqJRXnk0nTByLDNJE2bxh3DYlHscSQN8ypjdanv0zQj5mjBsB73aNuwfCpd4Sc1kVqcdeT8yHfP1RJe15X0Pu61RHUScw0qaRWm3FJ960yct2rwawspig0W4UiKRPVjIPAHILi3e+g2mo4py2BW0IwYEe+MAgAImYA4UYewNMIBhrAkJxgQiT+UZpDCD2h6yGDIoRrfx38VZYxgNcJ5xkrt4CocP4FKA0rkE3lDdslH8pZ8IX/GeiXKI6tlgKOda1nUmn12af3XkSofRwnuSDWxZgkduKVq9bD2SEWyXTi5v/0+e767WopuUpeka9Y/0uyQz7gDoL+T+f1Gqu+mFCPjfumOGfoOf7kEozlZ+/irD2RGSFngJnsPmLFLCE3wNwTda+2n2ALom648wtQ/ORCBKVDRfZxyBfthypUjlVXshymzaIpv1fz/ZR4EG5WyuViurN0oLt/LHy1Mw2W4AvP4Mm/CMjyCVaiDo13UlrQH2kP9vf5Z/6b/yKlT2lBzAfY1/fdfwpUK+A=</latexit> and , the gauged Lax pairs are

}

hL = e−(Z1−Z2)T2 hR = e−(Z1+Z2)T2 <latexit sha1_base64="8X4oSAI6sH/bR0Mz6Tlp/D+ElE=">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</latexit> for L for R ˆ L1 L = +F1(λ)dY, ˆ L2 L = −F1(λ) [dZ1 − dZ2 − cos Y (dZ1 + dZ2)] − (dZ1 − dZ2) , ˆ L3 L = +F1(λ) sin Y (dZ1 + dZ2) , ˆ L1 R = +F2(λ)dY, ˆ L2 R = +F2(λ) [dZ1 + dZ2 − cos Y (dZ1 − dZ2)] − (dZ1 + dZ2) ˆ L3 R = +F2(λ) sin Y (dZ1 − dZ2) <latexit sha1_base64="T7VBwN5Oazf+relEg6vfV9JKZE4=">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</latexit> F1() = [(ibλ − aλ) + (iaλ − bλ) ? ] F2() = [(ibλ + aλ) + (iaλ + bλ) ? ] <latexit sha1_base64="isMFOlLnazcLXo5xMWLXLJ0xCJk=">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</latexit> ☆ Remove the explicit dependence on ! (Z1, Z2) 13
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SLIDE 15
  • O(d, d)
  • 3. Doubled formalism

and

  • transformations

O(d, d)

  • Xi ˜

X i

slide-16
SLIDE 16

3.1 Setting of doubled formalism

\ Assume the following situation: Base manifold Torus fiber

Td

Adapted coords: Xi ( Killing vectors: ) ∂Xi Dual torus fiber

˜ Td

Dual coords: ˜ X i

}

Doubled torus

T2d

Doubled coords: 𝕐I = ( Xi ˜ X i )t ( cf: Buscher rule ) Local coords: Y [Hull] 15
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SLIDE 17

3.2 Action of doubled formalism

\ Doubled sigma model action: with the generalized metric HIJ = ✓G − BG−1B BG−1 −G−1B G−1 ◆ IJ <latexit sha1_base64="+XhKrvcpHR2gcyAP86Q0rSy5fA=">AD6HichVI9bxNBEB3n+AjmIw40SDQrLEc0tYBCYRARKZIQCkSByeWcsG6u2ziI/fF3drIrPwHqOgiREUkCsR/oKHhD1Ckp0EIhBQkGgre7TmKILEzq7t9+2be7Mzu2pHnJpLz3dyYceLkqdPjZ/Jnz52/MFGYvLichJ3YEQ0n9MK4aVuJ8NxANKQrPdGMYmH5tidW7K37qX+lK+LEDYNHsheJNd/aDNwN17EkqFahafqWbDuWp+b6LfXgYZ/dZXnGzMh/KntqlpVZbfaxKlf7NTa1D5lpImRgZXbgz1CWp1Uo8grXxg6D6gAU7/0kbQvhZO4OmbROITnUIZ8EBSBPbIowVilKnGKwK2RAhcDudovqE95aDuIEoiwG7hv4nV6oANsE5zJlrtYBcPXwloxL/zN/xPf6Jv+df+Z+huZTOkdbSw2xnWhG1Jl5cXvp9rMrHLKl9oBpZs6QNuqVrdVF7pJm0CyfTd59v7y3drpfUFN/h31D/G7LP6KDoPvLebso6q9H1GOjbwtrgZzDT06By86+jdX6yMgIMT140vtIdGQJsQF8z/RZ+7r7AFmUvuM0W4r2zyQGUprNdhmnMc4Sjl/rLKOcZQyZdO3Wv3/ZR4Gy9OV6vXK9OKN4kwte7Q0TlfoKl3Dy7xJMzRHC9TA3h/oC32nH8YT46WxbzKQsdyA80l+seMnb/mH+Mv</latexit> Let some act as g ∈ O(d, d) , then the action is invariant. H → gtHg, dX → g−1dX, J → gtJ <latexit sha1_base64="JT1+bC+r9XaKdSk7dxTD9PEK2L8=">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</latexit> X → g−1X, g ∈ O(d, d; Z) <latexit sha1_base64="HWnCa9VI3NICMSkLtePlpu0tiGI=">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</latexit> Note! : symmetry g ∈ O(d, d; R) <latexit sha1_base64="fzBG5GV+OleoiK4h9mlotSuISLQ=">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</latexit> : deformation (sol. generating tech.)

No

∈ O(d, d) <latexit sha1_base64="Y+X3IgxuvCtVYJFlvbC7SL8ZUw=">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</latexit> Xi <latexit sha1_base64="IrgHKjfkLTvBq2dw1JHAvk40PFE=">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</latexit> S = Z 1 2HIJ dXI ∧ ?dXJ + dXI ∧ ?JI(Y ) + L(Y ) <latexit sha1_base64="BMjPLcabaNm8V0jfgjQOKVAodUc=">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</latexit> [Hull] 16
slide-18
SLIDE 18

3.2 Action of doubled formalism

\ Doubled sigma model action: with the generalized metric HIJ = ✓G − BG−1B BG−1 −G−1B G−1 ◆ IJ <latexit sha1_base64="+XhKrvcpHR2gcyAP86Q0rSy5fA=">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</latexit> Let some act as g ∈ O(d, d) , then the action is invariant. H → gtHg, dX → g−1dX, J → gtJ <latexit sha1_base64="JT1+bC+r9XaKdSk7dxTD9PEK2L8=">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</latexit> X → g−1X, g ∈ O(d, d; Z) <latexit sha1_base64="HWnCa9VI3NICMSkLtePlpu0tiGI=">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</latexit> Note! : symmetry g ∈ O(d, d; R) <latexit sha1_base64="fzBG5GV+OleoiK4h9mlotSuISLQ=">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</latexit> : deformation (sol. generating tech.)

No

∈ O(d, d) <latexit sha1_base64="Y+X3IgxuvCtVYJFlvbC7SL8ZUw=">ADmHichVJNaxRBEH2b8SPGjyR6Eb0sLisRZOmNgUgIuJiDCgGTjZuEfBmZjtJk5meYWZ2ZR3yBzwHPIiCgfxZ3jxD3jIT5BcAhG8ePBNz4qYZDfdzHTVq3rVdXlhJ6KEyH2CwPWufMXLg5eGrp85eq14ZHR64tx0Ipc2XADL4iWHTuWntKykajEk8thJG3f8eSszOT2ZfaMopVoF8knVCu+/aWVpvKtRNCK2tKF5+PNe8372MlERFmFU8KVS7QunRIcyaC0YL01hDEwFctOBDQiOh7MFGzL2KgRCYutIiUWUlLFL7GKI3Ba9JD1sojv8b1Fb7aKaehYzNmyXt3j8IjKLKIv4rM4Et/EF/FD/O4ZKzUxslw6PJ2cK8ON4dc3F36dyfJ5Jtj+x+qbc4JNPDS5KuYeGiSrws357Vdvjham6uX0rvgoDpj/B7EvrIC3f7pfpqX9bd98nFYt01dMmbvzqXE8t5vU2v29Qzp06Ele4/YeJbpq2l7aXrtm+o1o6TmjbNomfS3JxGl1KD5Lb2Ys9ynMWfPZNa5T2Nm6C5ntXp8Mk8Ki+OV6oPK+PxEqfY4H1oM4jbuYIyTOYkanmIODd6tsYd3eG/dsmrWE+tZ7jpQ6HJu4L9l1f8AnIrJdg=</latexit> Xi <latexit sha1_base64="IrgHKjfkLTvBq2dw1JHAvk40PFE=">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</latexit> S = Z 1 2HIJ dXI ∧ ?dXJ + dXI ∧ ?JI(Y ) + L(Y ) <latexit sha1_base64="BMjPLcabaNm8V0jfgjQOKVAodUc=">AEMHichVLNaxNBFH/b1VrR1O9CF4WQ6RiCZP4iSgWvbQhzYxbaTbhtnNJFm6X+xOUuKw/4D/gAcvKngQb/4LXvwHBHsSj+pFqODFg29mE0TJDPszpvfe7/3Nc8KXSfmhBxoM/qx47Mn5k7Onzp95uxCZvHcZhx0I5vV7MANorpFY+Y6Pqtxh7usHkaMepbLtqy9h1K/1WNR7AT+I94P2Y5H27TcmzKEWpkXlSNe4bp+NwWxG1RSERxcQwPco7NnXFatIQa6XEXDbMZjOFLUvUk12xhlb7rNlmhlzGo3oS4lxdTpGKck4yRLj69I0hAsS6CRyZI8UcsYFQoDIXv/B6i1Hixqd8GEJgRgQxc8YOADR9kFCjHubSgAgRCxHRCIRSg5Ss8gXnkdtGKoQVFdA/bxtD1Af79JnrNg2RnHxi5BpQI58JG/IflA3pKv5PdYX0L5kLn08bRSLgsbC08vVH9NZXl4cuj8ZU3MmUMLbqtcHcw9VIiswk75vSfPDqt3Kjlxmbwi3zH/l+SAvMcK/N5P+/UGqzyfkI+FdVO8M/Q5vnMCsbT3Hbw1J1qGaNHjXyPWFnm0NZH3b7qtaeq9GLUG8svUlp2JMIJaHQNMo4Zhn3UczyVGYF91FMiSY4q4X/J3NU2CzmC9fyxY3r2ZUH6dDCHFyES7CEk3kLVmAV1qEGtjarLWs3tJv6O/2T/ln/kprOaAPOefhn6d/+AGKQAik=</latexit> ☆ deformations via field redefinition: O(d, d; ℝ) H(G, B) → gtHg = H(G0, B0), dX → g1dX = dX0 <latexit sha1_base64="rYsVOKQM3aD6HinwEagLeOBj9I=">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</latexit> [Hull] 16
slide-19
SLIDE 19 \ (Suppose that there is no source term) To get back to the sigma model from the doubled action
  • ne condition imposed (self-duality constraint) :
dXI = LIJHJK ? dXK <latexit sha1_base64="YpmnQsVeiTpnrfFnv7Thpca2iMk=">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</latexit> LIJ = ✓1 1 ◆ <latexit sha1_base64="x+2FIo9LTn8Ye3GTdu73cDhkU9A=">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</latexit> Unpackaging the constraint, d e Xi = ?
  • GijdXj + Bij ? dXj
= ?Ji <latexit sha1_base64="4+1FtdylfPsbnwhtvytBf1IFNZU=">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</latexit> ☆ The winding coordinates turn into
  • isometry currents.
U(1) ☆ leads to the conservation of (EOMs for ). d2˜ X i = 0 Ji Xi

}

EOMs for and 𝕐I Y + self-duality constraint

}

EOMs for and Xi Y
  • f physical sigma model
  • f doubled sigma model

3.3 Constraint on doubled formalism

[Hull] 17
slide-20
SLIDE 20 \ The transformation rule for under global : dXi O(d, d)

3.4 (-duality) map

O(d, d)

Start from with dX0 = g1dX <latexit sha1_base64="LGrjcAnl6uOaJxlDJEMRPHrmbU=">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</latexit> αi j, βij, γij, δi j <latexit sha1_base64="OuipnjSFcRMYFkuWgxI1qCpoqH0=">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</latexit> : matrices. d × d dXi = αi jdX0j + βijd e X0 j <latexit sha1_base64="RTWOEOPh2Q/QjdTEIPNwzUqMd0=">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</latexit> g = ✓α β γ δ ◆ <latexit sha1_base64="s7rNsRaFLIb7hsGd4klAsoLtdB4=">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</latexit> Then . Using the self-duality constraint, dXi = ↵i jdX0j + ij ? J0 j <latexit sha1_base64="D/dqs7vwcCzwLeIwl3m5+C0J0=">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</latexit> Thus, the action on Lax pairs: O(d, d) Gauging L − → ˆ L(dX) − → L0(dX0) = ˆ L(dX → D(dX0)) <latexit sha1_base64="3ur7HeiAl0+NB8wveF4Ck2oSgcY=">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</latexit> Just applied the map to the gauged Lax pairs! O(d, d) = Di(dX0) <latexit sha1_base64="vmNbZv3ZDcaC8GOfagQg0Je2/5U=">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</latexit> [Rennecke] 18
slide-21
SLIDE 21 \ Do
  • deformed Lax pairs satisfy zero-curvature condition?
O(d, d)

3.5 Flatness of

  • deformed Lax pairs

O(d, d)

19
slide-22
SLIDE 22 \ Do
  • deformed Lax pairs satisfy zero-curvature condition?
O(d, d)

3.5 Flatness of

  • deformed Lax pairs

O(d, d)

dL + L ∧ L = 0 <latexit sha1_base64="J9uKD1jafYfH0C6VAlZ8Kbq1KI=">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</latexit> (on-shell) 19
slide-23
SLIDE 23 \ Do
  • deformed Lax pairs satisfy zero-curvature condition?
O(d, d)

3.5 Flatness of

  • deformed Lax pairs

O(d, d)

Anyways, start from the curvature of Lax connections d ˆ L + ˆ L ∧ ˆ L = (EOMs) <latexit sha1_base64="jGpnyV2/JS1jKACtVQO0X7xHkU8=">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</latexit>
  • f the undeformed model
for and Xi Y 19
slide-24
SLIDE 24 \ Do
  • deformed Lax pairs satisfy zero-curvature condition?
O(d, d)

3.5 Flatness of

  • deformed Lax pairs

O(d, d)

Anyways, start from the curvature of Lax connections d ˆ L + ˆ L ∧ ˆ L = (EOMs) <latexit sha1_base64="jGpnyV2/JS1jKACtVQO0X7xHkU8=">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</latexit>
  • f the undeformed model
☆ The doubled action is invariant under . S = S′ O(d, d) for and Xi Y
  • 2. The EoMs for of the undeformed model
Xi →A linear combinations of EoMs for ‘s. X′i (thanks to the self-duality constraint) 19
  • 1. The EoM for of the undeformed model
Y → The EoM for of the deformed model. Y
slide-25
SLIDE 25 \

3.5 Flatness of

  • deformed Lax pairs

O(d, d)

Start from with dX0 = g1dX <latexit sha1_base64="LGrjcAnl6uOaJxlDJEMRPHrmbU=">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</latexit> αi j, βij, γij, δi j <latexit sha1_base64="OuipnjSFcRMYFkuWgxI1qCpoqH0=">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</latexit> : matrices. d × d The transformation rule for under global : d˜ X i O(d, d) Then . d e Xi = γijdX0j + δi kd e X0 k <latexit sha1_base64="yTSxfGgd+8z+EwodxySZM/ivTh8=">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</latexit> Using the self-duality constraint, ?Ji = ijdX0j + i k ? J0 k <latexit sha1_base64="EDTJQ1y6ve8Nhm5j23k0zsqrxTs=">AEBXichVLPa9RAFH5p/FG3ard6EbwEl62CsMy2giKRS8iPbRbt1oapgk023c/CLJrqwhZ8F/wIMnBQ8i3sSrBy/+Ax6Kf4F4ESp48eA3kxXRdrczJPeN9/3puZ8e+l2aM7WpT+pGjx45Pn6jMnDx1erY6d2Y9jfqJI9pO5EdJx+ap8L1QtDMv80UnTgQPbF9s2L07cn9jIJLUi8L72TAWwHvht625/AMkFXtm2nGE+OelXuFMX/TMLs8CDi8h4Vhuq7RMVWOPBFucXFk2z53esWDHJTLIAk/k4IiB9SDqgw4VmeBZFVrMHUMPYbzZFRu/Wd1FiJ5rQbZJLETnUp4AEhZTB9olTirlJTWIUA9uiHFgCy1P7gqQNsHS4DBgfbw78LbHKEhfBkzVWoHWXx8CZQG1dln9prtsU/sDfvKfo2NlasYspYhVrvUitiafXpu7ehqgBrRjt/VRNrzmibrqlaPdQeK0Sewin1g8fP9taut+r5PHvJvqH+F2yXfcQJwsEP59WqaD2fUI+Nc3P4AjH31wOrLz7HXjuRGYMzhA78j1SxayDG2LvkbrQJ0+RJRcvbGMJq0/d5LAyhVaZhmnXMY8SLl8qLKFeZBSorJXm/935n5jfaHRXGwsrF6pLd0um5am6TxdoEvozKu0RHdphdrI/UXTtIo2oz/R3+rv9PcldUobac7SP0P/8BvGk/UP</latexit> g = ✓α β γ δ ◆ <latexit sha1_base64="RXari4rZzFOr020XjIVNHhVJ9kU=">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</latexit> 20
slide-26
SLIDE 26 \

3.5 Flatness of

  • deformed Lax pairs

O(d, d)

Start from with dX0 = g1dX <latexit sha1_base64="LGrjcAnl6uOaJxlDJEMRPHrmbU=">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</latexit> αi j, βij, γij, δi j <latexit sha1_base64="OuipnjSFcRMYFkuWgxI1qCpoqH0=">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</latexit> : matrices. d × d The transformation rule for under global : d˜ X i O(d, d) Then . d e Xi = γijdX0j + δi kd e X0 k <latexit sha1_base64="yTSxfGgd+8z+EwodxySZM/ivTh8=">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</latexit> Using the self-duality constraint, g = ✓α β γ δ ◆ <latexit sha1_base64="RXari4rZzFOr020XjIVNHhVJ9kU=">AD13ichVLNaxNBFH/p+lHrR1O9CF4WQ4qnMGkFRLe9BD21q2kq3hNnNFk6uzvuTiLpEnoT8ebJgycFDyL+FV68i4eC/gHiRajgxYO/nY340SadYXfe/N7va95rpJ+ohnbK4xZx46fODl+auL0mbPnJotT51eTqBN7ou5FMorXZ4I6Yeirn0txbqKBQ9cKdbc7YVMv9YVceJH4T3dU2Iz4K3Q3/I9rgE1inda9i3bUcED3Uth0vV5va07bhCc9txbMdESF3ZEX2nxYPAaP8Gm0LCtN8oliFmWUfFKoDoXT7G5m1FE0VbpJDTYrIow4FJCgkDVkSpwR7g6rESAHbpBRYDMk3ekF9mgC3AysBCw50G/8WbhsDNMQ985kYtocoEl8Mpk1l9pG9ZvsPXvDvrCfQ32lxkeWSw+nm3OFakw+ubjy40hWgFNT+w9rZM6atui6ydVH7sogWRVezu/uPNtfuVErp9PsJfuK/F+wPfYOFYTd796rZVF7PiIfF3Vz3AV8Du9cCizvfRu35khLBZseNl7JMayDNsQuoem14GpPoSX1Lx5i2TfvckhpQaNI8yjLmIfRhz8UhmDfswZoZms1r9fzIPCqszlepsZWb5amluPh9aGqdLdJmuYDKv0RzdpSWqI/Zb+kCf6LN139q1HlmPc9OxwoBzgf5Z1tNfdObi7g=</latexit> Field equations of the original model are mapped to those
  • f the deformed model.
Zero-curvature conditions guaranteed after transformations O(d, d)

d ? Ji = i k d ? J0 k <latexit sha1_base64="UZwqPpJGoAthWEZwvkx/wScHlQ=">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</latexit> 20
slide-27
SLIDE 27
  • JJ
  • 4. Application
slide-28
SLIDE 28 \

4.1 (current-current) deformation

J ¯ J

Marginal deformation by the operator of Deformed U(1) currents in the Cartan subalgbera S(α+δα) − S(α) ∼ δα π f(α) Z d2zJ(α)J(α) <latexit sha1_base64="hPbhWThELqXz0EHCBnYyl/SfHFM=">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</latexit> Deformed generalized metric obtained by the matrix O(2,2) g =     1 tan α 1 1+tan α tan α 1+tan α 1 1+tan α 1 1+tan α −1 1     <latexit sha1_base64="1hKGcI/0SIU5DG9/Ttv0Jk4ubPw=">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</latexit> in the basis of XI = ⇣ Z1, Z2, e Z1, e Z2 ⌘t <latexit sha1_base64="m9VJ5Zh5YZo012ogop7G3gt4SzI=">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</latexit> gtH(G, B)g = H(G0, B0) <latexit sha1_base64="Iu82Zn8OsDNwGzEabdtro6sYqQ=">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</latexit> Deformed background data obtained via field redefinition [Hassan, Sen] 22
slide-29
SLIDE 29 \

4.1 (current-current) deformation

J ¯ J

Given the matrix and deformed background data, O(2,2) apply the map to : . O(2,2) (dZ1, dZ2) dXi = ↵i jdX0j + ij ? J0 j <latexit sha1_base64="X7a0Ue6j9hGonCaEhya+khYL9DU=">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</latexit>

}

dZ1 = dZ0 1 + tan ↵ ? J2(↵) dZ2 = 1 1 + tan ↵ [dZ0 2 − tan ↵ ? J1(↵)] <latexit sha1_base64="/Aof38RXYbpIj8zbBMtzjNuKD6o=">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</latexit> g =     1 tan α 1 1+tan α tan α 1+tan α 1 1+tan α 1 1+tan α −1 1     <latexit sha1_base64="1hKGcI/0SIU5DG9/Ttv0Jk4ubPw=">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</latexit> 23
slide-30
SLIDE 30 \

4.1 (current-current) deformation

J ¯ J

Given the matrix and deformed background data, O(2,2) apply the map to : . O(2,2) (dZ1, dZ2) dXi = ↵i jdX0j + ij ? J0 j <latexit sha1_base64="X7a0Ue6j9hGonCaEhya+khYL9DU=">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</latexit>

}

dZ1 = dZ0 1 + tan ↵ ? J2(↵) dZ2 = 1 1 + tan ↵ [dZ0 2 − tan ↵ ? J1(↵)] <latexit sha1_base64="/Aof38RXYbpIj8zbBMtzjNuKD6o=">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</latexit> g =     1 tan α 1 1+tan α tan α 1+tan α 1 1+tan α 1 1+tan α −1 1     <latexit sha1_base64="1hKGcI/0SIU5DG9/Ttv0Jk4ubPw=">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</latexit> ˆ L1 L = +F1(λ)dY, ˆ L2 L = −F1(λ) [dZ1 − dZ2 − cos Y (dZ1 + dZ2)] − (dZ1 − dZ2) , ˆ L3 L = +F1(λ) sin Y (dZ1 + dZ2) , ˆ L1 R = +F2(λ)dY, ˆ L2 R = +F2(λ) [dZ1 + dZ2 − cos Y (dZ1 − dZ2)] − (dZ1 + dZ2) ˆ L3 R = +F2(λ) sin Y (dZ1 − dZ2) <latexit sha1_base64="T7VBwN5Oazf+relEg6vfV9JKZE4=">AHpnictVLNahNRFD6p0dT40YRBDcXQ0pKNdykiKRaG4CNKmpmbiXF+bpIhk8kwcxOJ47yAL+DClQUXUt/CjS/go8gboQKblx45k5qrcmkU8EZkjn3PN9zvnfopl6A6ndDc2dSJ+8lRi+nTyzNlz52dmUxfWnW7PVlZ7Rpde0ORHWboJitznRtsw7KZ3FEMVlHaD/39Sp/Zjt41n/CBxWoduWnqDV2VOabqfglqSVzV+rIvKXKhlv0vKdu3qu7UrHokbl7ZIEs1zGRlQwk1eR5Imka2bwmSckxwMIfwOsjQIM1eJVIQrRrM83zqb8omFOMWS17SFytKYwrsYhmwFrNgLrQgRWydabLT4fGr+IVHZo2gesofMbnHi0B3d/E/NopzqTYvXxmkSRiVAk3LPsUxfBCGi2qDQz2Q302QyEYgUe4qlHg4HjLJDAcnkH/Rvm+3cD+EzTDMDqGCjtWzJNVn0zRHxUNGg/wSN/BuJZ6aZid0ECDbqgQg86wMAEjrEBMj4ViEPFCzM1cDFnI2RLvYZeJBEbA+rGFbImG3jfxNX1WHWxLXP6Qi0iqcY+LMRSBDP9P3dI9+ojv0C/0ZyuUKDl/LAL9KgGVWfebV5bUfR6I6+OXQOkBN1MyhAbeFVh21WyLjd6EG+P6L13trd0oZd45u06+o/y3dpR+xA7P/X23ykpvJuhRsG8Z1w5wyfnYi6YfQtX2sRKC2sGuOPfhyMqM1hr4t5zMeuO6N5EFlfcsc/mR/szsTFyRTY4JQxZxHcsngksoTvOKSf9dCr+b+dORqsF3L5xVxh9UZ6UFgWpiGK3AVsujMW7AEj2AFyqDGX8a34zvxD4ls4nGinKgEpVOxIeYiHoSz34BIgtDYA=</latexit> 23
slide-31
SLIDE 31 \

4.1 (current-current) deformation

J ¯ J

Given the matrix and deformed background data, O(2,2) apply the map to : . O(2,2) (dZ1, dZ2) dXi = ↵i jdX0j + ij ? J0 j <latexit sha1_base64="X7a0Ue6j9hGonCaEhya+khYL9DU=">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</latexit>

}

g =     1 tan α 1 1+tan α tan α 1+tan α 1 1+tan α 1 1+tan α −1 1     <latexit sha1_base64="1hKGcI/0SIU5DG9/Ttv0Jk4ubPw=">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</latexit> dL0 + L0 ∧ L0 = 0 <latexit sha1_base64="HCVluv2Pkm45V+wLRfixi2g18G8=">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</latexit> still holds. dZ1 = dZ0 1 + tan ↵ ? J2(↵) = D1(dZ0) dZ2 = 1 1 + tan ↵ [dZ0 2 − tan ↵ ? J1(↵)] = D2(dZ0) <latexit sha1_base64="0Ww+IMXmsfNuGzs8le3pmwcHAwI=">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</latexit> L01 L = +F1(λ)dY, L02 L = −F1(λ) [D1(dZ0) − D2(dZ0) − cos Y (D1(dZ0) + D2(dZ0))] − (D1(dZ0) − D2(dZ0)) , L03 L = +F1(λ) sin Y (D1(dZ0) + D2(dZ0)) , L01 R = +F2(λ)dY, L02 R = +F2(λ) [D1(dZ0) + D2(dZ0) − cos Y (D1(dZ0) − D2(dZ0))] − (D1(dZ0) + D2(dZ0)) , L03 R = +F2(λ) sin Y (D1(dZ0) − D2(dZ0)) . <latexit sha1_base64="J6vBSeHsfEqUBXMV3xbkaJ9McjU=">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</latexit> 23
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SLIDE 32
  • 5. Conclusions and Outlook
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SLIDE 33 \

5 Conclusions and Outlook

This work completed the classical integrability of any global
  • transformation using the doubled formalism.
O(d, d; ℝ) Possible future directions: ☆ What type of algebra of non-local charges? ☆ The map for the spectral parameter ? O(d, d) λ ☆ The classical integrability of doubled formalism itself? Beyond global : O(d, d; ℝ) ☆ Extension to local transformations? O(d, d; ℝ) (What would be a collective T-duality invariant framework…?) → classical integrability of non-geometric backgrounds 25 [Kawaguchi, Matsumoto, Yoshida] [work in progress] [Kawaguchi, Yoshida]
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SLIDE 34

Thank you!