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arXiv math-ph/0505039math-phhep-thmath.DGmath.MPnlin.SI
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分裂号差下的整体反自对偶Yang-Mills场及其散射

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

L. J. Mason

AI总结:

本文将Ward的ASDYM扭量构造适配到分裂号差的共形紧化Minkowski空间二重覆叠上,建立整体解与扭量数据的一一对应,并构造了ASDYM场的散射映射。

摘要:

我们研究了分裂号差下反自对偶Yang-Mills(ASDYM)方程的解,这些解在相应共形紧化Minkowski空间的二重覆叠$\tilde{M}$上是整体的。通过建立$\tilde{M}$的点与扭量空间$\text{CP}^3$中边界落在实切片$\text{RP}^3$上的全纯圆盘之间的对应关系,我们将Ward的ASDYM扭量构造适配到了这一几何结构中。我们得到了$\tilde{M}$上ASDYM方程的光滑整体$\text{U}(n)$解与一对对象之间的一一对应:这对对象包括$\text{CP}^3$上的任意全纯向量丛$E$,以及$E$在$\text{RP}^3$上的限制$E|_{\text{RP}^3}$上的光滑正定埃尔米特度量$H$。丛$E$没有拓扑或其他方面的限制。这一描述推广了1+1维可积系统散射变换的结果:在1+1维情形中,解被编码为代数数据(此处对应$E$)与反射系数(此处对应$H:\text{RP}^3\to E\bar\bigotimes E$)的组合。对于平凡丛$E$,扭量数据由$\text{RP}^3$上的光滑埃尔米特矩阵函数$H$(差常数因子意义下)构成;此时的对应关系给出了X射线变换的一种非线性推广。我们还给出了具有不同$E$拓扑的显式例子。我们建立了分裂号差下ASDYM场的散射问题,并证明:通过取一族和乐,再进行两次Birkhoff分解,过去无穷远处足够小的数据可以唯一确定未来无穷远处的数据。散射映射在和乐层面是简单的,但在非阿贝尔情形下,在联络层面是非平凡的。

英文摘要:

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.

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