Integrals of periodic motion for classical equations of relativistic string with masses at ends

Details Integrals of periodic motion for classical equations of relativistic string with masses at ends Integrals of periodic motion for classical equations of relativistic string with masses at ends

1997-12-03

arxiv.org/abs/hep-th/9712030v1

Nucl.Phys.Proc.Suppl. 57 (1997) 284-287

Physics

High Energy Physics

High Energy Physics - Theory

8 pages, REVTEX, no figures and tables

Scientific paper

10.1016/S0920-5632(97)00405-2

Boundary equations for the relativistic string with masses at ends are formulated in terms of geometrical invariants of world trajectories of masses at the string ends. In the three-dimensional Minkowski space $E^1_2$, there are two invariants of that sort, the curvature $K$ and torsion $\kappa$. For these equations of motion with periodic $\kappa_i(\tau+n l)=\kappa(\tau)$, constants of motion are obtained.

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