The post-Newtonian Hamiltonian of an atom in a weak gravitational field is derived from first principles, and its center-of-mass motion matches a point particle whose mass is the total mass-energy of the atom.
Quantum interferometric visibility as a witness of general relativistic proper time,
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Post-Newtonian Hamiltonian description of an atom in a weak gravitational field
The post-Newtonian Hamiltonian of an atom in a weak gravitational field is derived from first principles, and its center-of-mass motion matches a point particle whose mass is the total mass-energy of the atom.