...
首页> 外文期刊>Journal of High Energy Physics >Tree-level S-matrix of Pohlmeyer reduced form of AdSn 5 × Sn 5 superstring theory
【24h】

Tree-level S-matrix of Pohlmeyer reduced form of AdSn 5 × Sn 5 superstring theory

机译:Pohlmeyer的树级S矩阵简化形式的AdSn 5×Sn 5超弦理论

获取原文
获取原文并翻译 | 示例
           

摘要

With a motivation to find a 2-d Lorentz-invariant solution of the AdS 5 × S 5 superstring we continue the study of the Pohlmeyer-reduced form of this theory. The reduced theory is constructed from currents of the superstring sigma model and is classically equivalent to it. Its action is that of G/H = Sp(2, 2) × Sp(4)/[SU(2)]4 gauged WZW model deformed by an integrable potential and coupled to fermions. This theory is UV finite and is conjectured to be related to the superstring theory also at the quantum level. Expanded near the trivial vacuum it has the same elementary excitations (8+8 massive bosonic and fermionic 2-d degrees of freedom) as the AdS 5 × S 5 superstring in the S 5 light-cone gauge or near plane-wave expansion. In contrast to the superstring case, the interaction terms in the reduced action are manifestly 2-d Lorentz invariant. Since the theory is integrable, its S-matrix should be effectively determined by the two-particle scattering. Here we explicitly compute the tree-level two-particle S-matrix for the elementary excitations of the reduced theory. We find that this S-matrix has the same index structure and group factorization properties as the superstring S-matrix computed in hep-th/0611169 but has simpler coefficients, depending only on the difference of two rapidities. While the gauge-fixed form of the reduced action has only the bosonic [SU(2)]4 part of the PSU(2|2) × PSU(2|2) symmetry of the light-cone superstring spectrum as its manifest symmetry we conjecture that it should also have a hidden fermionic symmetry that effectively interchanges bosons and fermions and which should guide us towards understanding the relation between the two S-matrices.
机译:为了找到AdS 5×S 5超弦的2维Lorentz不变解,我们继续研究Pohlmeyer简化形式的该理论。归约理论是根据超弦西格玛模型的潮流而构建的,在经典意义上等同于它。它的作用是G / H = Sp(2,2)×Sp(4)/ [SU(2)] 4规范的WZW模型,该模型通过可积势变形并耦合到费米子。该理论是紫外线有限的,并且推测在量子水平上也与超弦理论有关。它在微不足道的真空附近扩展,具有与S 5光锥度规或近平面波扩展中的AdS 5×S 5超弦相同的基本激发(8 + 8大质量的正弦波和费米子2维自由度)。与超弦情况相反,减少动作中的相互作用项显然是二维洛伦兹不变的。由于该理论是可积分的,因此应通过两粒子散射有效地确定其S矩阵。在这里,我们为简化理论的基本激发显式计算树级两粒子S矩阵。我们发现,此S矩阵与在hepth / 0611169中计算的超字符串S矩阵具有相同的索引结构和组分解特性,但系数更简单,这仅取决于两个速度的差异。虽然规矩固定形式的减少作用仅具有圆锥形超弦谱的PSU(2 | 2)×PSU(2 | 2)对称性的玻色[SU(2)] 4部分作为其明显的对称性,但我们推测它还应该具有隐藏的费米子对称性,可以有效地交换玻色子和费米子,并且应该指导我们理解两个S矩阵之间的关系。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号