SCOAP3 Repository 6 records found  Search took 0.01 seconds. 
1. Handling Handles: Nonplanar Integrability in N=4 Supersymmetric Yang-Mills Theory / Bargheer, Till ; Caetano, João ; Fleury, Thiago ; Komatsu, Shota ; et al
We propose an integrability setup for the computation of correlation functions of gauge-invariant operators in N=4 supersymmetric Yang-Mills theory at higher orders in the large Nc genus expansion and at any order in the ’t Hooft coupling gYM2Nc. [...]
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: two-particle contributions / Fleury, Thiago ; Komatsu, Shota
In this work, we compute one-loop planar five-point functions in N = 4 $$ \mathcal{N}=4 $$ super-Yang-Mills 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 single-trace operators in N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills 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 three-point functions of single-trace operators in the s u 1 | 1 $$ \mathfrak{s}\mathfrak{u}\left(1\Big|1\right) $$ 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. Three-point functions and s u 1 | 1 $$ \mathfrak{s}\mathfrak{u}\left(1\Big|1\right) $$ spin chains / Caetano, João ; Fleury, Thiago
We compute three-point functions of general operators in the s u 1 | 1 $$ \mathfrak{s}\mathfrak{u}\left(1\Big|1\right) $$ sector of planar N $$ \mathcal{N} $$ = 4 SYM in the weak coupling regime, both at tree-level and one-loop. [...]
Published in JHEP 1409 (2014) 173 10.1007/JHEP09(2014)173 arXiv:1404.4128
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See also: similar author names
1 Fleury, T.
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