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We point out that in this work we make use of the heuristic time-energy uncertainty principle (Ref.) rather than the rigorous inequality by Mandelshtam and Tamm
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We point out that in this work we make use of the heuristic time-energy uncertainty principle (Ref.) rather than the rigorous inequality by Mandelshtam and Tamm [L. I. Mandelshtam and I. E. Tamm, J. Phys. (USSR) 9, 249 (1945)]. Our goal here is indeed to merely estimate the characteristic time scale Δτ over which entanglement builds up. A more accurate quantification of such a time is under ongoing investigation.
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We assume that | μ̄ belongs to the uncoupled-spin basis { |μ□ }. The generalization to arbitrary (pure or mixed) initial spin states is straightforward.
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We assume that | μ̄ belongs to the uncoupled-spin basis { |μ□ }. The generalization to arbitrary (pure or mixed) initial spin states is straightforward.
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We numerically trace over the spatial variable using a mesh of the region where fe (x,τ) is non negligible and checking the stability of the outcomes vs the number of mesh points.
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We numerically trace over the spatial variable using a mesh of the region where fe (x,τ) is non negligible and checking the stability of the outcomes vs the number of mesh points.
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The monotonic rise of entanglement observed in Figs. clearly depends on the initial spin state (if the static spins are already entangled, a decrease may take place).
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The monotonic rise of entanglement observed in Figs. clearly depends on the initial spin state (if the static spins are already entangled, a decrease may take place).
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