Contact interaction in Lagrangians

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SUMMARY

The discussion focuses on the variation of an action involving two point particles coupled by a delta function contact interaction in D-dimensional space. The action is expressed as S = ∫ dt (1/2) dot{x}² + ∫∫ dt dot{x}(t) δ^D(x(t) - y(t')) dot{y}(t') dt' + ∫ dt' (1/2) dot{y}². The participants conclude that while integrating the delta function is feasible in D=1, complications arise in higher dimensions. The challenge lies in correctly performing the variation of the delta function term, particularly when accounting for the intersection of particle worldlines.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with delta function properties in physics
  • Knowledge of variations in field theory
  • Experience with D-dimensional space concepts
NEXT STEPS
  • Study the properties of delta functions in higher dimensions
  • Learn about variations in Lagrangian field theory
  • Explore the implications of gauge fixing in particle actions
  • Investigate the mathematical treatment of point particle interactions
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The discussion is beneficial for theoretical physicists, particularly those specializing in classical mechanics, field theory, and particle interactions. It is also relevant for graduate students studying advanced topics in physics.

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Hi all,

If I take an action involving two point particles coupled together by a delta function contact interaction is it possible to carry out the variation with respect to the fields? For e.g.

[itex] S = \int dt \frac{1}{2} \dot{x}^{2} + \int \int dt \dot{x}(t) \delta^{D}\left(x(t) - y(t')\right) \dot{y}(t')dt' + \int dt' \frac{1}{2}\dot{y}^{2}<br /> [/itex]

working in, say, D dimensions. I think it will be possible to integrate the delta function out in D=1, but not in higher target space dim. The problem I have is in how to do the variation of the delta function term. Physically it is producing an interaction every time the worldlines of the particles intersect and I've tried writing this as a sum over such points - where [itex]x(t_{0})=y(t')[/itex] - of [itex]\frac{\delta(t - t_{0})}{\dot{x}(t_{0})}[/itex] but this is valid only in D = 1 and I still can't get the variation correct.

Any help would be appreciated.
I
 
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where are your space integral parts.If you are doing a one dimensional problem then you will have D=1,if you are doing a D dimensional one your eqn will be modified and the effect of delta function is to just make x(t)=y(t') in second integral after space integration but nevertheless what you have written for first integral and third (not to mention second one) just does not qualify.
 
There are no space integrals - it is a (gauge fixed) action for point particles, proportional to the length of the worldline in D dimensional target space plus some interaction terms. The domain is one dimensional, as for the ordinary relativistic point particle.

Sorry for the confusion
I
 

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