If the solution of a field vanishes on-shell does it mean anything?

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SUMMARY

The discussion centers on the implications of a field's solution vanishing on-shell, specifically for the field ##c## in the action ##S=S(a,b,c)##. When the fields ##a## and ##b## satisfy their equations of motion, the condition ##f(a,b)=0## indicates that field ##c## has no independent dynamics and is entirely determined by ##a## and ##b##. This on-shell condition serves as a constraint on the system's dynamics and may also arise from underlying symmetries or conservation laws within the action.

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  • Understanding of functional actions in field theory
  • Knowledge of equations of motion for fields
  • Familiarity with on-shell and off-shell conditions
  • Concept of symmetries in physical systems
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  • Study the implications of on-shell conditions in classical field theories
  • Explore the role of symmetries in determining field dynamics
  • Investigate the relationship between conservation laws and field constraints
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The discussion is beneficial for theoretical physicists, particularly those focusing on field theory, as well as graduate students studying dynamics and symmetries in physical systems.

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Let us consider an action ##S=S(a,b,c)## which is a functional of the fields ##a,\, b,\,## and ##c##. The solution of the field ##c## is given by the expression ##f(a,b)##. On taking into account the relations obtained from the solutions for ##a## and ##b##, we find that ##f(a,b)=0##. If the solution for the field ##c## vanishes on-shell, does it mean anything particular?
 
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Yes, the fact that the solution for the field ##c## vanishes on-shell has a specific meaning in this context. It means that when the fields ##a## and ##b## satisfy the equations of motion, the field ##c## automatically satisfies the equation ##f(a,b)=0##. This is known as the on-shell condition for the field ##c##.

Physically, this on-shell condition indicates that the field ##c## does not have any independent dynamics and its behavior is completely determined by the fields ##a## and ##b##. This can be interpreted as a constraint on the dynamics of the system, where the value of ##c## is completely determined by the values of ##a## and ##b## at every point in spacetime.

In some cases, the on-shell condition for a field may also arise due to symmetries or conservation laws in the system. For example, if the action ##S## is invariant under a certain symmetry transformation, then the on-shell condition for the corresponding field would be a consequence of this symmetry.

In summary, the vanishing of the solution for a field on-shell has a significant meaning and can provide insights into the dynamics and symmetries of the system.
 

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