Integrating geological, geochemical and geophysical data and uncertainties into a coherent 3D model

Geoneutrino measurements by particle physicists provide the opportunity for geoscientists to build interdisciplinary
\nbridges to solve open questions about heat production in our planet. Geoneutrinos are electron antineutrinos emitted
\nin beta minus decays, with some from the 238U and 232Th decay chains having sufficient energy to be detected.
\nThese particles, originating from the crust and the mantle, are able to pass through most matter without interacting,
\nso they can bring to surface useful information about the planet’s composition. Their detection establishes the
\nplanet’s radioactive element budget. Experimental results from ongoing (KamLAND and Borexino) and future experiments
\n(e.g., SNO+, JUNO, Jinping) broaden their value if supported by a priori geophysical and geochemical
\nmodels based on an integrated understanding and quantification of uncertainties. The mantle contribution to the
\ngeoneutrino signal at an individual detector cannot be pursued without critically combining multi-source uncertainties
\naffecting the modeling and evaluating their correlation.
\nThanks to 2 km of rock overburden and ~1 kiloton of ultrapure liquid scintillator, the SNO+ detector (Ontario,
\nCanada) is strategically designed for detecting low energy anti-neutrinos, and aims to reach several fundamental
\nphysics goals, among them the study of geoneutrinos. The geoneutrino signal produced by U and Th distributed is
\ndominated by the closest lithologies in the surrounding 50 x 50 km of upper crust near SNO+ whose contribution
\nis comparable with that of the whole mantle of the Earth. We focused on this crucial portion of Canadian Shield,
\nand characterized nine distinct units based on lithology, metamorphism, tectonic events, and evolutional history.
\nWe developed a 3D numerical model defined by multiple geological and geophysical inputs (e.g., geological map,
\ndigital elevation models, cross sections deriving from seismic and gravimetric inputs) and the estimation error was
\ninferred on the base of probabilistic geostatistical methods. A sampling campaign that was proportionally biased to
\nthe surface area distribution of lithologies and a statistical study of the frequency distributions, allowed for probing
\nthe normal and lognormal tendencies of the U and Th distributions, providing for each unit the central value and
\nthe uncertainties of the abundances.
\nUncertainties in the predicted geoneutrino signal were estimated considering the degree of correlation between
\nvalues for U and Th abundances. Monte Carlo simulations were conducted in order to propagated uncertainties
\nassuming a bivariate normal distribution for the Probability Density Function’s (PDF) describing the joint logarithmic
\nU and Th distribution. The mentioned geochemical PDFs combined with the geophysical uncertainties are
\nthe input for building the total geoneutrino signal distributions from which the median and 1σ values are derived.

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