000625630 001__ 625630 000625630 005__ 20250410223119.0 000625630 037__ $$aPUBDB-2025-01156 000625630 041__ $$aEnglish 000625630 1001_ $$0P:(DE-H253)PIP1101735$$aLai, Davide$$b0$$eCorresponding author$$udesy 000625630 1112_ $$aQFT, Strings and Beyond$$cZürich$$d2025-03-18 - 2025-03-18$$wSwitzerland 000625630 245__ $$aClustering and the Five-Point Function$$f2025-03-18 - 000625630 260__ $$c2025 000625630 3367_ $$033$$2EndNote$$aConference Paper 000625630 3367_ $$2DataCite$$aOther 000625630 3367_ $$2BibTeX$$aINPROCEEDINGS 000625630 3367_ $$2ORCID$$aLECTURE_SPEECH 000625630 3367_ $$0PUB:(DE-HGF)31$$2PUB:(DE-HGF)$$aTalk (non-conference)$$btalk$$mtalk$$s1744271560_3645143$$xInvited 000625630 3367_ $$2DINI$$aOther 000625630 502__ $$cETH Zürich 000625630 520__ $$aThe hexagonalisation technique arose in the context of N=4 SYM theory to address the tessellation of the effective world-sheet describing three-point functions of single trace operators. Despite its apparent technical difficulty, exploiting the knowledge of all its ingredients at finite 't Hooft coupling one can perform some non-trivial limits, like the strong-coupling one. In this case, a phenomenon called "clustering" allows the complete resummation of finite-size effects leading to the semi-classical string answer. I will introduce the general background and then discuss the generalization to some particular class of five-point functions, where the clustering phenomenon becomes more involved, involving cross-ratios and some analytic continuation of the ingredients to unusual kinematic regimes. In the end, I will speculate about some tentative directions that one could take. 000625630 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0 000625630 536__ $$0G:(GEPRIS)460391856$$aDFG project G:(GEPRIS)460391856 - Feldtheorie lösen mittels Integrabilität (460391856)$$c460391856$$x1 000625630 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0 000625630 8564_ $$uhttps://seminars.itp.phys.ethz.ch/view?series=qftstrbyd&period=25FS 000625630 8564_ $$uhttps://bib-pubdb1.desy.de/record/625630/files/Slides.pdf$$yRestricted 000625630 8564_ $$uhttps://bib-pubdb1.desy.de/record/625630/files/Slides.pdf?subformat=pdfa$$xpdfa$$yRestricted 000625630 909CO $$ooai:bib-pubdb1.desy.de:625630$$pVDB 000625630 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1101735$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY 000625630 9131_ $$0G:(DE-HGF)POF4-611$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vFundamental Particles and Forces$$x0 000625630 9141_ $$y2025 000625630 9201_ $$0I:(DE-H253)T-20120731$$kT$$lTheorie-Gruppe$$x0 000625630 980__ $$atalk 000625630 980__ $$aVDB 000625630 980__ $$aI:(DE-H253)T-20120731 000625630 980__ $$aUNRESTRICTED