For particle positions , the two-particle Schrodinger equation isWrite for the localized wave packet and . Neglecting packet spreading and branch overlap, the initial product state evolves branchwise asup to phases generated independently on the two particles. These branch-dependent phases generally cannot be separated into one phase depending only on and one depending only on , so the Newtonian gravitational potential energy creates gravitationally induced entanglement.
If is much smaller than the other separations, remove their nearly common phase and retain onlyThe state is approximatelyIts concurrence is , so it becomes maximally entangled first at . For ,Thus the near-maximal entanglement time is about within the stated approximation.
A single prescribed classical gravitational potential gives a Hamiltonian of the form . Its evolution factorizes as and preserves every initial product state, so it cannot generate this entanglement. A semiclassical mean field sourced only by expectation values likewise gives each particle a local one-body potential and does not provide a quantum mediator carrying branch correlations.
An entanglement witness is a Hermitian operator whose expectation is nonnegative on every separable state but negative on at least one entangled state. At , defineThe largest Schmidt coefficient of is , so every product state in the four-dimensional branch subspace satisfies . By closure under convex combinations, for every separable mixture, whereasA negative measured value therefore certifies entanglement. Under the assumptions that the masses began unentangled and interacted only through gravity, such certification would show that the mediator can transmit quantum coherence; it would be evidence against a purely classical gravitational channel and for the quantum nature of gravity.
Articles by others on the same topic
There are currently no matching articles.