Why are objective collapse theories stated to collapse the state from a superposition to a single eigenstate (corresponding to the measured eigenvalue)? For this discussion, we are focusing on the mathematics of the equations, not on any interpretation on quantum mechanics. I merely wish to know if objective collapse equations (the dynamics as described by the typically stochastic differential equations) yield something like: (a) \begin{equation} \langle x\mid \rho(t)\mid y\rangle \propto e^{-\lambda(x-y)^2 t}\langle x\mid \rho(0)\mid y\rangle \end{equation} or (b) \begin{equation} \langle x\mid \rho(t)\mid y\rangle \propto e^{-\lambda((x-x_0)^2+(y-x_0)^2) t}\langle x\mid \rho(0)\mid y\rangle \end{equation} where the system tends to the pure state $\mid x_0\rangle \langle x_0\mid $, where $x_0$ is the randomly measured eigenvalue.
In (a), we have a process which can be achieved via a Lindblad equation derived from an open quantum system. In this context the process would be termed "decoherence".If we find (a), then I find the name "objective collapse" to be inappropriate because I would define collapse as in (b). Hence, the second question is whether anyone actually uses the term "collapse" for the process in (a).