This work demonstrates how time arises from the constraint geometry in bilocal phase space, revealing new insights into relational dynamics.
The aim of this work is to show that the notion of time can be derived from theconstraint geometry of a bilocal phase space. The starting point is neither timenor a Hamiltonian, but rather the relation between two configurations, its phasespace, the symplectic form, and the constraint. We show locally that the transition to relational variables leads to the decomposition \[Δ^a=t n^a,^an_a=1,\] and in phase space to the dual decomposition \[Π^2=p_t^2+L^2/t^2.\] The bilocal constraint then takes the form \[C=Qₑₓₜ(X,P)-p_t^2-L^2/t^2=0.\] After restricting the symplectic form to the constraint surface, we obtain apresymplectic form whose kernel is one-dimensional. Consequently, the constraintsurface is foliated by one-dimensional orbits, and the variable \(t\) can beinterpreted as a parameter of these orbits, that is, as relational time.
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Andrzej Tyminski (2026) studied this question.
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