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Global anti-self-dual Yang-Mills fields in split signature and their scattering

L. J. Mason

TL;DR

The paper develops a global Ward-type correspondence for anti-self-dual Yang-Mills fields in split signature, tying smooth ASDYM connections on the double cover of conformally compactified space to pairs (E,H) of a holomorphic vector bundle on twistor space and a Hermitian metric on its real slice. It then interprets the nonlinear X-ray transform in this non-linear, twistor-theoretic setting and constructs a nonlinear scattering theory for small data via holonomies and two Birkhoff factorizations, showing that the scattering is generically nontrivial in the non-abelian case. Through explicit Abelian and non-Abelian examples, including Ward/t’Hooft ansatze and split-signature instantons, the work clarifies how topological data (c1,c2,c3,α-invariants) manifest in space-time fields and how twistor data encodes both radiative and solitonic content. The results illuminate the rich structure of ASDYM in split signature and suggest connections to twistor-string theory and higher-dimensional integrable systems. Overall, the paper provides a complete geometric framework for global split-signature ASDYM solutions and their nonlinear scattering, expanding the toolbox for twistor methods in gauge theory.

Abstract

We consider solutions to the anti-self-dual Yang Mills (ASDYM) equations in split signature that are global on the double cover of the appropriate conformally compactified Minkowski space $\widetilde\M$. Ward's ASDYM twistor construction is adapted to this geometry by using a correspondence between points of $\widetilde\M$ and holomorphic discs in $\CP^3$, twistor space, with boundary on the real slice $\RP^3$. A 1-1 correspondence is obtained between smooth global $\U(n)$ solutions to the ASDYM equations on $\widetilde\M$ and pairs consisting of an arbitrary holomorphic vector bundle $E$ over $\CP^3$ together with a smooth positive definite hermitian metric $H$ on $E|_{\RP^3}$. There are no topological or other restrictions on the bundle $E$. The description generalises the result of the scattering transform for 1+1 dimensional integrable systems in which solutions are encoded into a combination of algebraic data, here $E$, and a reflection coefficient, here $H:\RP^3\to E\otimes\bar E$. For trivial $E$, the twistor data consists of the smooth Hermitian matrix function $H$ on $\RP^3$ up to constants; the correspondence then provides a nonlinear generalisation of the X-ray transform. Explicit examples are given with different topologies of $E$. A scattering problem for ASDYM fields in split signature is set up and it is shown that sufficiently small data at past infinity uniquely determines data at future infinity by taking a family of holonomies followed by a sequence of two Birkhoff factorizations. The scattering map is simple on the holonomies, but non-trivial at the level of the connection in the non-abelian case.

Global anti-self-dual Yang-Mills fields in split signature and their scattering

TL;DR

The paper develops a global Ward-type correspondence for anti-self-dual Yang-Mills fields in split signature, tying smooth ASDYM connections on the double cover of conformally compactified space to pairs (E,H) of a holomorphic vector bundle on twistor space and a Hermitian metric on its real slice. It then interprets the nonlinear X-ray transform in this non-linear, twistor-theoretic setting and constructs a nonlinear scattering theory for small data via holonomies and two Birkhoff factorizations, showing that the scattering is generically nontrivial in the non-abelian case. Through explicit Abelian and non-Abelian examples, including Ward/t’Hooft ansatze and split-signature instantons, the work clarifies how topological data (c1,c2,c3,α-invariants) manifest in space-time fields and how twistor data encodes both radiative and solitonic content. The results illuminate the rich structure of ASDYM in split signature and suggest connections to twistor-string theory and higher-dimensional integrable systems. Overall, the paper provides a complete geometric framework for global split-signature ASDYM solutions and their nonlinear scattering, expanding the toolbox for twistor methods in gauge theory.

Abstract

We consider solutions to the anti-self-dual Yang Mills (ASDYM) equations in split signature that are global on the double cover of the appropriate conformally compactified Minkowski space . Ward's ASDYM twistor construction is adapted to this geometry by using a correspondence between points of and holomorphic discs in , twistor space, with boundary on the real slice . A 1-1 correspondence is obtained between smooth global solutions to the ASDYM equations on and pairs consisting of an arbitrary holomorphic vector bundle over together with a smooth positive definite hermitian metric on . There are no topological or other restrictions on the bundle . The description generalises the result of the scattering transform for 1+1 dimensional integrable systems in which solutions are encoded into a combination of algebraic data, here , and a reflection coefficient, here . For trivial , the twistor data consists of the smooth Hermitian matrix function on up to constants; the correspondence then provides a nonlinear generalisation of the X-ray transform. Explicit examples are given with different topologies of . A scattering problem for ASDYM fields in split signature is set up and it is shown that sufficiently small data at past infinity uniquely determines data at future infinity by taking a family of holonomies followed by a sequence of two Birkhoff factorizations. The scattering map is simple on the holonomies, but non-trivial at the level of the connection in the non-abelian case.

Paper Structure

This paper contains 27 sections, 12 theorems, 56 equations.

Key Result

Theorem 1

Gauge equivalence classes of $C^\infty$ solutions to the ASDYM equations on $\widetilde{\mathbb{M}}$ are in 1-1 correspondence with principal $G_\mathbb{C}$ bundles $P\rightarrow \mathbb{PT}$ together with a $C^\infty$ reduction of the structure group to $G$ over $\mathbb{PT}_\mathbb{R}$ where $G_\m

Theorems & Definitions (14)

  • Theorem 1
  • Lemma 2.1
  • Corollary 2.1
  • Theorem 2
  • Lemma 3.1
  • Lemma 3.2
  • Theorem 3
  • Theorem 4
  • Definition 5.1
  • Definition 5.2
  • ...and 4 more