We study the interplay of squeezing and phase randomization near the hyperbolic instability of a two-site Bose-Hubbard model in the Josephson interaction regime. We obtain results for the quantum Zeno suppression of squeezing far beyond the previously found short time behavior. More importantly, we contrast the expected outcome with the case where randomization is induced by erratic driving with the same fluctuations as the quantum noise source, finding significant differences. These are related to the distribution of the squeezing factor, which has log-normal characteristics: hence its average is significantly different from its median due to the occurrence of rare events.
I. INTRODUCTIONThe effect of stochastic driving on unitary evolution has been a central theme of modern quantum mechanics. It is well established that quantum decay can be suppressed by frequent interventions, or measurements, or by the introduction of noise, via the Quantum Zeno Effect (QZE) [1][2][3][4][5][6][7][8][9][10][11][12]. The modelling of the "interventions" as arising from a deterministic or from a noisy source are often used interchangeably [5][6][7][8][9]. This partially reflects the paradigm that the Langevin picture and the Master equation picture of the dynamics are equivalent.Recent work considered the QZE suppression of interaction-induced squeezing in bimodal Bose-Einstein condensates [13,14]. Since matter-wave squeezing is the key to the realization of atom interferometers below the standard quantum limit [15][16][17][18][19][20], it is highly desirable to gain better understanding of its interplay with noise. Noise was shown to arrest the squeezing and build-up of many-body correlations in the large, multi-particle system, prepared with all particles occupying the odd superposition of the two-modes. In the Josephson regime [21] this preparation constitutes a hyperbolic saddle point, leading to a rapid squeezing [22,23]. It was shown that the degree of squeezing and the associated phase diffusion [24][25][26][27][28][29] could be controlled by a noisy modulation of the coupling between the modes, up to a full arrest via a Bose-stimulated QZE [13,14].In this work we attain two principle goals. (i) We extend the analytic understanding of the QZE suppression of squeezing to time-scales which are orders of magnitude longer than these of Ref. [13,14], obtaining good agreement with numerical simulations. (ii) We challenge the fundamental paradigm of replacing quantum noise by deterministic erratic driving. Erratic driving can have nontrivial statistics, hence its typical results do not have to agree with the average behavior. This is demonstrated in our system by an important caveat resulting from the interplay of the nonlinear squeezing dynamics and the diffusive randomization by driving. While the early evolution under the influence of either noisy or erratic driving corresponds to the QZE of Ref. [13,14], significant differences arise at later times. These differences are explained by a statistical analysis: As the squeezing...