Controlling measurement-induced phase transitions with tunable detector coupling
1Department of Physics, Ben Gurion University of the Negev, Israel
2Department of Physics, Lancaster University, United Kingdom
3Université Paris-Saclay, CNRS, Laboratoire de Physique des Solides, 91405, Orsay, France.
| Published: | 2025-04-08, volume 9, page 1697 |
| Editor: | Angelo Carollo |
| Eprint: | arXiv:2404.07918v4 |
| Doi: | https://doi.org/10.22331/q-2025-04-08-1697 |
| Citation: | Quantum 9, 1697 (2025). |
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Abstract
We study the evolution of a quantum many-body system driven by two competing measurements, which induces a topological entanglement transition between two distinct area law phases. We employ a positive operator-valued measurement with variable coupling between the system and detector within free fermion dynamics. This approach allows us to continuously track the universal properties of the transition between projective and continuous monitoring. Our findings suggest that the percolation universality of the transition in the projective limit is unstable when the system-detector coupling is reduced.

Featured image: (a) Space-time schematic of two competing measurements $\hat{M}^D$, $\hat{M}^K$ on the Majorana (free fermionic) chain. The two partitions of chains A and B contribute to calculating topological entanglement entropy. (b) The probability distribution of the detector outcome $x$ is modified by the coupling to the system. The modified probability distribution $ P(x)$ depends on the coupling strength ($\sqrt{\gamma dt}$).
Popular summary
At one extreme—strong, projective measurements—the system behaves like a classical percolation model, where entanglement is broken into isolated clusters that percolate at the transition. At the other extreme, weak and continuous monitoring—entanglement spreads more freely, as the observer causes minimal disturbance to the system’s state while also gathering very little information on average.
A key finding is that the mathematical characteristics of this transition evolve as measurement strength is tuned. In particular, the "correlation length exponent," which describes how correlations scale near the transition, steadily increases as the system moves away from the projective limit. This suggests that the classical percolation picture, valid under strong measurements, fails to describe the system as monitoring becomes weaker.
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