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Color-kinematics duality from an algebra of superforms

Roberto Bonezzi, Christoph Chiaffrino, Olaf Hohm, Maria Foteini Kallimani

TL;DR

This work introduces a novel algebraic framework to derive color-kinematics (CK) duality from first principles by embedding the Yang-Mills (YM) kinematic sector into the algebra of superforms on a superspace, endowed with a strict $BV^{\square}$ algebra and its BV$_{\infty}^{\square}$ generalization. By partitioning the de Rham complex into an ideal up to homotopy and taking a quotient, the color-stripped YM $C_{\infty}$ algebra emerges with a nontrivial $m_3$ that encodes YM interactions, while the quotient carries the YM kinematic structure. The bracket $b_2=[b,m_2]$ realizes a Lie-like structure up to higher homotopies, with the CK duality at tree level arising because the Jacobiator is cancelled by higher maps such as $b_3$ and $ heta_3$, rendering the obstruction exact and removable by multiparticle gauge transformations. The program outlines an algorithmic path to determine higher BV$_{\infty}^{\square}$ maps, aiming to derive gravity as the double copy from YM data and to extend the construction to more elaborate theories, including supersymmetric variants.

Abstract

Color-kinematics duality states that the kinematic numerators of the cubic tree-level Yang-Mills scattering amplitudes obey the same symmetry properties that the color factors obey due to the Jacobi identity. We present a novel strategy for deriving this duality, based on the differential forms on a superspace. This space of superforms carries a generalization of a Batalin-Vilkovisky (BV) algebra (BV$^{\square}$ algebra). We show that the homotopy algebra of color-stripped Yang-Mills theory is obtained as a quotient of this space in which a subspace, which is an ideal `up to homotopy', is modded out. This algebra is a subsector of a BV$_{\infty}^{\square}$ algebra. Deriving the latter would provide a first-principle proof of color-kinematics duality from field theory.

Color-kinematics duality from an algebra of superforms

TL;DR

This work introduces a novel algebraic framework to derive color-kinematics (CK) duality from first principles by embedding the Yang-Mills (YM) kinematic sector into the algebra of superforms on a superspace, endowed with a strict algebra and its BV generalization. By partitioning the de Rham complex into an ideal up to homotopy and taking a quotient, the color-stripped YM algebra emerges with a nontrivial that encodes YM interactions, while the quotient carries the YM kinematic structure. The bracket realizes a Lie-like structure up to higher homotopies, with the CK duality at tree level arising because the Jacobiator is cancelled by higher maps such as and , rendering the obstruction exact and removable by multiparticle gauge transformations. The program outlines an algorithmic path to determine higher BV maps, aiming to derive gravity as the double copy from YM data and to extend the construction to more elaborate theories, including supersymmetric variants.

Abstract

Color-kinematics duality states that the kinematic numerators of the cubic tree-level Yang-Mills scattering amplitudes obey the same symmetry properties that the color factors obey due to the Jacobi identity. We present a novel strategy for deriving this duality, based on the differential forms on a superspace. This space of superforms carries a generalization of a Batalin-Vilkovisky (BV) algebra (BV algebra). We show that the homotopy algebra of color-stripped Yang-Mills theory is obtained as a quotient of this space in which a subspace, which is an ideal `up to homotopy', is modded out. This algebra is a subsector of a BV algebra. Deriving the latter would provide a first-principle proof of color-kinematics duality from field theory.
Paper Structure (5 sections, 33 equations, 1 figure)

This paper contains 5 sections, 33 equations, 1 figure.

Figures (1)

  • Figure 1: Bicomplex of superforms. The degrees $(p,q)$ in the above diagram are given by $(N,G-N)$. The spaces that descend to the Yang-Mills kinematic algebra ${\cal K}$ are displayed in green. Spaces in gray are zero, due to $c^2=0$.