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Dirac constraint analysis and symplectic structure of anti-self-dual Yang-Mills equations

机译:反自对偶Yang-Mills方程的Dirac约束分析和辛结构

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We present the explicit form of the symplectic structure of anti-self-dual Yang-Mills (ASDYM) equations in Yang's J- and K-gauges in order to establish the bi-Hamiltonian structure of this completely integrable system. Dirac's theory of constraints is applied to the degenerate Lagrangians that yield the ASDYM equations. The constraints are second class as in the case of all completely integrable systems which stands in sharp contrast to the situation in full Yang-Mills theory. We construct the Dirac brackets and the symplectic 2-forms for both J- and K-gauges. The covariant symplectic structure of ASDYM equations is obtained using the Witten-Zuckerman formalism. We show that the appropriate component of the Witten-Zuckerman closed and conserved 2-form vector density reduces to the symplectic 2-form obtained from Dirac's theory. Finally, we present the Baecklund transformation between the J- and K-gauges in order to apply Magri's theorem to the respective two Hamiltonian structures.
机译:为了建立这个完全可积系统的双哈密尔顿结构,我们提出了在杨氏J量规和K量规中反自对偶Yang-Mills(ASDYM)方程的辛结构的显式形式。狄拉克的约束理论适用于产生ASDYM方程的退化拉格朗日方程。与所有完全可积分的系统一样,这些约束是第二类的,这与完整的Yang-Mills理论的情况形成鲜明对比。我们为J和K规构造Dirac括号和辛2形式。使用Witten-Zuckerman形式主义获得ASDYM方程的协变辛结构。我们表明,Witten-Zuckerman闭合且守恒的2型矢量密度的适当分量降低为从Dirac理论获得的辛2型。最后,我们提出了J量规和K量规之间的Baecklund变换,以便将Magri定理应用于相应的两个哈密顿量结构。

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