We propose a model to identify the quantum/classical boundary. The model introduces a spontaneous collapse of state superposition: $\frac{d}{dt} \rho_{ij} =-\frac{i}{\hbar}[H,\rho]{ij}-\rho{ij}/\tau_{ij}$. Different from other collapse models, the collapsing scale here does not contain a universal parameter, but is specified by the two states and $ | j\rangle$: If each state is {\em in principle} repeatedly readable (typically by a QND measurement), then is the {\em potentially} needed measuring time to discriminate the two states, and the collapse occurs spontaneously {\em without} any actual monitoring. Otherwise, , 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{"o}dinger’s cat”, the superposition of and is forbidden if , and allowed if , where is the trap separation and is the energy gap, which can be estimated with . The model also constrains a “free Schr{"o}dinger’s cat” to display double-slit interference if , where $p= Mv\theta D$ 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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