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Scattering Amplitudes from the Amplituhedron NMHV Volume Forms

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Scattering Amplitudes from the Amplituhedron NMHV Volume Forms Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Scattering amplitudes from the amplituhedron NMHV volume forms Andrea Orta Ludwig-Maximilians-Universit¨atM¨unchen V Postgraduate Meeting on Theoretical Physics Oviedo, 17th November 2016 Based on 1512.04954 with Livia Ferro, TomaszLukowski, Matteo Parisi Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Table of contents 1 Scattering amplitudes in planar N = 4 super Yang-Mills Heavy computations for simple amplitudes N = 4 SYM 2 Introduction to the tree-level Amplituhedron Positive geometry Amplitudes as volumes 3 NMHV volume forms from symmetry Capelli differential equations The k = 1 solution Examples of NMHV volume forms 4 Conclusions Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Scattering amplitudes . Scattering amplitudes are central objects in QFT. Interesting as an intermediate step to compute observables; as a means to gain insight into the formal structure of a specific model. How are they traditionally computed? 1 Stare at Lagrangian and extract the Feynman rules; 2 draw every possible Feynman diagram contributing to the process of interest; 3 evaluate each one of those and add up the results. Straightforward enough. What could possibly go wrong? Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry . are complicated? Consider tree-level gluon amplitudes in QCD. 2g ! 2g : 4 diagrams Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry . are complicated? Consider tree-level gluon amplitudes in QCD. 2g ! 3g : 25 diagrams [slide by Z. Bern] Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry . are simpler than expected! Consider tree-level gluon amplitudes in QCD. 2g ! 3g : 10 colour-ordered diagrams tree ± ± ± ± ± A5 (1 ; 2 ; 3 ; 4 ; 5 ) = 0 tree ∓ ± ± ± ± A5 (1 ; 2 ; 3 ; 4 ; 5 ) = 0 h12i4 Atree(1−; 2−; 3+; 4+; 5+) = 5 h12ih23ih34ih45ih51i + − 3 1 1 2 α β λi λj hiji = αβλi λj = 2 2 + λi λj 4 1− 5+ Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry . are simpler than expected! Consider tree-level gluon amplitudes in QCD. 2g ! 3g : 10 colour-ordered diagrams tree ± ± ± ± ± A5 (1 ; 2 ; 3 ; 4 ; 5 ) = 0 tree ∓ ± ± ± ± A5 (1 ; 2 ; 3 ; 4 ; 5 ) = 0 h12i4 Atree(1−; 2−; 3+; 4+; 5+) = 5 h12ih23ih34ih45ih51i hiji4 AMHV(1+;:::; i −;:::; j−;:::; n+) = n h12ih23i · · · hn1i MHV = maximally helicity-violating [Parke, Taylor] (Ordinary + Dual) superconformal symmetries give rise to an infinite-dimensional Yangian algebra Y psu(2; 2j4) [Drummond, Henn, Plefka] At weak coupling : more constrained, easier to compute At strong coupling : amenable to AdS/CFT techniques Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The simplest quantum field theory [Arkani-Hamed, Cachazo, Kaplan] Most symmetric theory in 4D is planar N = 4 super Yang-Mills. Maximal susy: spectrum is organized in a single supermultiplet with 2 gluons (g ±), 8 gluinos ( ±), 6 scalars ('), all massless. 1 Ω = g + + ηA + ηAηB' + A 2 AB 1 1 + ηAηBηC ¯ D + ηAηBηCηD g − 3! ABCD 4! ABCD Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The simplest quantum field theory [Arkani-Hamed, Cachazo, Kaplan] Most symmetric theory in 4D is planar N = 4 super Yang-Mills. Maximal susy: spectrum is organized in a single supermultiplet with 2 gluons (g ±), 8 gluinos ( ±), 6 scalars ('), all massless. (Ordinary + Dual) superconformal symmetries give rise to an infinite-dimensional Yangian algebra Y psu(2; 2j4) [Drummond, Henn, Plefka] At weak coupling : more constrained, easier to compute At strong coupling : amenable to AdS/CFT techniques planar N =4 SYM N =4 SYM SYM massless massive [picture by L. Dixon] Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The simplest quantum field theory [Arkani-Hamed, Cachazo, Kaplan] Most symmetric theory in 4D is planar N = 4 super Yang-Mills. Maximal susy: spectrum is organized in a single supermultiplet with 2 gluons (g ±), 8 gluinos ( ±), 6 scalars ('), all massless. (Ordinary + Dual) superconformal symmetries give rise to an infinite-dimensional Yangian algebra Y psu(2; 2j4) [Drummond, Henn, Plefka] At weak coupling : more constrained, easier to compute At strong coupling : amenable to AdS/CFT techniques N = 4 SYM is a supersymmetric version of QCD: Tree-level gluon amplitudes coincide One-loop gluon amplitudes satisfy QCD N =4 N =1 scalar An = An − 4An + An Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The power of momentum twistors \Masslessness" of the spectrum + conformal symmetry −! introduce momentum supertwistors for describing the kinematics. Instead of four-momenta pµ µ = 0; 1; 2; 3 and Grassmann-odd ηA A = 1; 2; 3; 4 α; α_ = 0; 1; 0_; 1_ use mom. supertwistors ZA A = A = 1; 2; 3; 4 3j4 The geometry of momentum twistor superspace CP ensures masslessness of momenta and momentum conservation. Generating function for every tree-level N = 4 SYM amplitude Z 1 dk×nc L = αi δ4j4(C ·Z) n;k GL(k) (1 ··· k)(2 ··· k + 1) ··· (n ··· k − 1) [(Arkani-Hamed, Cachazo, Cheung, Kaplan) (Mason, Skinner)] Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Towards the amplituhedron Two remarkable results inspired the amplituhedron: 1 Z dk×nc L = αi δ4j4(C ·Z) n;k GL(k) (1 ··· k)(2 ··· k + 1) ··· (n ··· k − 1) One-to-one correspondence between residues of Ln;k and cells of the positive Grassmannian G+(k; n). [Arkani-Hamed, Bourjaily, Cachazo, Goncharov, Postnikov, Trnka] NMHV tree-level amplitudes can be thought of as volumes of polytopes in twistor space. [Hodges] Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry 1 Scattering amplitudes in planar N = 4 super Yang-Mills Heavy computations for simple amplitudes N = 4 SYM 2 Introduction to the tree-level Amplituhedron Positive geometry Amplitudes as volumes 3 NMHV volume forms from symmetry Capelli differential equations The k = 1 solution Examples of NMHV volume forms 4 Conclusions Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Positive means inside Z2 Y 2 Z3 Triangle in RP Z1 Interior of a triangle A A A A Y = c1Z1 + c2Z2 + c3Z3 ; c1; c2; c3 > 0 Points inside are described by the positive triple (c1 c2 c3)=GL(1) Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Positive means inside Y n−1 Simplex in RP Interior of a simplex A X A Y = ci Zi ; ci > 0 i Points inside are described by the positive n-tuple (c1 c2 ::: cn)=GL(1) , a point in G+(1; n) : Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Positive also means convex Z4 Z5 Y Polygon in m Zn RP Z3 Z1 Z2 Interior of a n-gon with vertices Z1;:::; Zn is only canonically defined if 0 1 1 1 1 Z1 Z2 ::: Zn B . C Z = @ . A 2 M+(1 + m; n) 1+m 1+m 1+m Z1 Z2 ::: Zn Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Tree-level amplituhedron m Interior of an n-polyhedron in RP ( ) tree A X A C = (c1 ::: cn) 2 G+(1; n) A [Z] = Y = ci Z ; n;1;m i Z = (Z ::: Z ) 2 M (1 + m; n) i 1 n + Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Tree-level amplituhedron m Interior of an n-polyhedron in RP ( ) tree A X A C = (c1 ::: cn) 2 G+(1; n) A [Z] = Y = ci Z ; n;1;m i Z = (Z ::: Z ) 2 M (1 + m; n) i 1 n + Generalize this picture to account for Nk MHV amplitudes Tree-level amplituhedron tree C 2 G+(k; n) An;k;m[Z] = Y 2 G(k; k+m): Y = C·Z ; Z 2 M+(k + m; n) [Arkani-Hamed,Trnka] Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The volume form Volume form ~ (m) tree Top-dimensional differential form Ωn;k defined on An;k;m with only logarithmic singularities on its boundaries. ~ (m) top-dimensional: Y 2 G(k; k + m) −! Ωn;k is an mk-form dα log-singularity : approaching any boundary, Ω~ (m) ∼ n;k α Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The volume form Volume form ~ (m) tree Top-dimensional differential form Ωn;k defined on An;k;m with only logarithmic singularities on its boundaries. ~ (m) top-dimensional: Y 2 G(k; k + m) −! Ωn;k is an mk-form dα log-singularity : approaching any boundary, Ω~ (m) ∼ n;k α Z2 If Y = α1Z1 + α2Z2 + Z3 ; Y Z 2 2 3 ~ (2) dα1 dα2 1 h123i hY d Y i Ω3;1 = ^ = α1 α2 2 hY 12ihY 23ihY 31i Z1 Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry The volume form Volume form ~ (m) tree Top-dimensional differential form Ωn;k defined on An;k;m with only logarithmic singularities on its boundaries. ~ (m) top-dimensional: Y 2 G(k; k + m) −! Ωn;k is an mk-form dα log-singularity : approaching any boundary, Ω~ (m) ∼ n;k α Z2 If Y = α1Z1 + α2Z2 + Z3 ; Y 2 Z3 (2) 1 h123i Ω3;1 = ≡ [1 2 3] Z 2 hY 12ihY 23ihY 31i 1 | {z } Area of (dual) triangle Amplitudes in planar N = 4 SYM Introduction to the tree-level Amplituhedron NMHV volume forms from symmetry Get to the amplitude Morally .
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