Repeatedly readable state, spontaneous collapse, and quantum/classical boundary

preprint2022arXivOpen access

Abstract

We propose a model to identify the quantum/classical boundary. The model introduces a spontaneous collapse of state superposition: ddtρij=−iℏ[H,ρ]ij−ρij/τij\frac{d}{dt} ρ_{ij} =-\frac{i}{\hbar}[H,ρ]_{ij}-ρ_{ij}/τ_{ij}. Different from other collapse models, the collapsing scale τijτ_{ij} here does not contain a universal parameter, but is specified by the two states ∣i⟩| i\rangle and ∣j⟩ | j\rangle: If each state is {\em in principle} repeatedly readable (typically by a QND measurement), then τijτ_{ij} is the {\em potentially} needed measuring time to discriminate the two states, and the collapse occurs spontaneously {\em without} any actual monitoring. Otherwise, τij=∞τ_{ij}=\infty, which means no collapse and everlasting superposition. This happens if one state is not repeatedly readable, or if the two states cannot possibly be discriminated in a particular circumstance (for example in the Rabi oscillation). Detailed analysis shows that for a "trapped Schr{ö}dinger's cat", the superposition of ∣here⟩|{\rm here} \rangle and ∣there⟩| {\rm there} \rangle is forbidden if ED≫4πℏcE D \gg 4π\hbar c, and allowed if ED≤4πℏcE D \le 4π\hbar c, where DD is the trap separation and E E is the energy gap, which can be estimated with Mv2 M v^2. The model also constrains a "free Schr{ö}dinger's cat" to display double-slit interference if pθD≥8ℏpθD\ge 8\hbar, where p=Mvp= Mv, θθ is the angle spanned by the two trajectories, and DD is the slit separation. In contrast, this model sets no limit on the coherent length of massless photon, thus the arm of a Michelson interferometer can be arbitrarily long. The spontaneous collapse which we propose can occur for an isolated system, and parallels the decoherence induced by interaction with environment.

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