Experimental exclusion of a generalized Károlyházy gravity-induced decoherence model
Nicola Bortolotti, Kristian Piscicchia, Matthias Laubenstein, Simone Manti, Antonino Marcianò, Federico Nola, Catalina Curceanu
TL;DR
The paper addresses gravity-induced decoherence models, specifically a generalized Károlyházy framework with a Gaussian spatial correlation length $R_K$. It uses the VIP germanium detector data from the LNGS underground laboratory and a Bayesian spectral analysis to search for spontaneous radiation signatures predicted by the model, incorporating detailed background modeling and material-dependent emission rates. The main result is a 95% CL lower bound of $R_K>4.64$ m, which, when considered alongside a theoretical upper bound $R_K<1.98$ m, excludes the entire generalized model and its non-Markovian CSL equivalence. This demonstrates the power of low-background underground experiments to constrain foundational quantum-mechanics modifications linked to gravity, and it highlights the potential for future, more stringent tests of non-Markovian collapse and gravity-related decoherence scenarios.
Abstract
We report new experimental constraints on the generalized version of the gravity-induced decoherence model originally proposed by Károlyházy. Using data collected by the VIP Collaboration at the INFN Gran Sasso National Laboratory with a high-purity germanium detector, we derive an improved lower bound on the spatial correlation length $R_K$ characterizing metric fluctuations in the model. We obtain a bound $R_K > 4.64$ m (95\% C.L.), which exceeds by more than an order of magnitude the previous experimental limit. When combined with the theoretical upper bound $R_K <1.98$ m derived from macroscopic localization requirements, our result excludes the generalized Károlyházy model. The same conclusion applies to an associated non-Markovian formulation of the Continuous Spontaneous Localization (CSL) model. Our findings significantly tighten experimental constraints on gravity-related decoherence scenarios and demonstrate the sensitivity of underground low-background experiments to foundational modifications of quantum mechanics.
