We consider a toy model for the study of monitored dynamics in many-body quantum systems. We study the stochastic Schrödinger equation resulting from continuous monitoring with a rate
of a random Hermitian operator, drawn from the Gaussian unitary ensemble (GUE) at every
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We consider a toy model for the study of monitored dynamics in many-body quantum systems. We study the stochastic Schrödinger equation resulting from continuous monitoring with a rate
of a random Hermitian operator, drawn from the Gaussian unitary ensemble (GUE) at every time
t. Due to invariance by unitary transformations, the dynamics of the eigenvalues
of the density matrix decouples from that of the eigenvectors, and is exactly described by stochastic equations that we derive. We consider two regimes: in the presence of an extra dephasing term, which can be generated by imperfect quantum measurements, the density matrix has a stationary distribution, and we show that in the limit of large size
it matches with the inverse-Marchenko–Pastur distribution. In the case of perfect measurements, instead, purification eventually occurs and we focus on finite-time dynamics. In this case, remarkably, we find an exact solution for the joint probability distribution of
’s at each time
t and for each size
n. Two relevant regimes emerge: at short times
, the spectrum is in a Coulomb gas regime, with a well-defined continuous spectral distribution in the
limit. In that case, all moments of the density matrix become self-averaging and it is possible to exactly characterize the entanglement spectrum. In the limit of large times
, one enters instead a regime in which the eigenvalues are exponentially separated
, but fluctuations
play an essential role. We are still able to characterize the asymptotic behaviors of the entanglement entropy in this regime.
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