子散射在自我双重的dyon上
Tim Adamo1, Giuseppe Bogna2, Lionel Mason2
1School of Mathematics and Maxwell Institute for Mathematical Sciences, University of Edinburgh, Peter Guthrie Tait Road, Edinburgh, EH9 3FD UK.
概括
我们得出了一个紧的公式,用于在自我双离子背景中的子的散射幅度. 这简化了量子场论中的计算,显示了不变形的分割函数和形代数.
科学领域:
- 量子场理论 量子场理论
- 高能物理 高能物理
- 弦理论中的弦理论.
背景情况:
- 在复杂的背景测量场中计算散射振幅是具有挑战性的.
- 奇拉背景字段为简化提供了一个有前途的途径.
- 以前的方法在多颗粒过程的明确公式方面遇到了困难.
研究的目的:
- 为了获得树级,最大螺旋体违反 (MHV) 子散射幅度的紧表达式.
- 分析自我双离子背景对这些振幅的影响.
- 在这个背景下调查可整合性和扰乱扩张.
主要方法:
- 利用扭曲子理论来利用自我双离子背景的整合性.
- 开发一个任意数量的质子的公式.
- 分析得到的散射振幅表达式.
主要成果:
- 在自我双离子背景中获得了MHV子散射幅度的紧公式.
- 该公式涉及单个位置空间积分,简化了计算.
- 发现全态对线分离函数是未变形的.
结论:
- 自带双离子背景简化了MHV部门的扰动性扩张.
- 未变形的分割函数意味着未变形的全态天体运算子的积分扩展和奇拉代数.
- 衍生式提供了一种途径,可以将计算扩展到完整的树级质子S矩阵.
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