1.

Handling Handles: Nonplanar Integrability in $N=4$ Supersymmetric YangMills Theory
/ Bargheer, Till ; Caetano, João ; Fleury, Thiago ; Komatsu, Shota ; et al
We propose an integrability setup for the computation of correlation functions of gaugeinvariant operators in $N=4$ supersymmetric YangMills theory at higher orders in the large ${N}_{c}$ genus expansion and at any order in the ’t Hooft coupling ${g}_{\mathrm{YM}}^{2}{N}_{c}$. [...]
Published in Physical Review Letters 121 (2018)
10.1103/PhysRevLett.121.231602
arXiv:1711.05326
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2.

Hexagonalization of correlation functions II: twoparticle contributions
/ Fleury, Thiago ; Komatsu, Shota
In this work, we compute oneloop planar fivepoint functions in N = 4 $$ \mathcal{N}=4 $$ superYangMills using integrability. [...]
Published in JHEP 1802 (2018) 177
10.1007/JHEP02(2018)177
arXiv:1711.05327
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3.

Hexagonalization of correlation functions
/ Fleury, Thiago ; Komatsu, Shota
We propose a nonperturbative framework to study general correlation functions of singletrace operators in N $$ \mathcal{N} $$ = 4 supersymmetric YangMills theory at large N . [...]
Published in JHEP 1701 (2017) 130
10.1007/JHEP01(2017)130
arXiv:1611.05577
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4.

Fermionic correlators from integrability
/ Caetano, João ; Fleury, Thiago
We study threepoint functions of singletrace operators in the s u 1  1 $$ \mathfrak{s}\mathfrak{u}\left(1\Big1\right) $$ sector of planar N = 4 $$ \mathcal{N}=4 $$ SYM borrowing several tools based on Integrability. [...]
Published in JHEP 1609 (2016) 010
10.1007/JHEP09(2016)010
arXiv:1607.02542
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5.

On the pure spinor heterotic superstring b ghost
/ Fleury, Thiago
A simplified pure spinor superstring b ghost in a curved heterotic background was constructed recently. [...]
Published in JHEP 1603 (2016) 200
10.1007/JHEP03(2016)200
arXiv:1512.00807
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6.

Threepoint functions and s u 1  1 $$ \mathfrak{s}\mathfrak{u}\left(1\Big1\right) $$ spin chains
/ Caetano, João ; Fleury, Thiago
We compute threepoint functions of general operators in the s u 1  1 $$ \mathfrak{s}\mathfrak{u}\left(1\Big1\right) $$ sector of planar N $$ \mathcal{N} $$ = 4 SYM in the weak coupling regime, both at treelevel and oneloop. [...]
Published in JHEP 1409 (2014) 173
10.1007/JHEP09(2014)173
arXiv:1404.4128
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