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Reference Models for Lithospheric Geoneutrino Signal

Identifikátory výsledku

  • Kód výsledku v IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216208%3A11320%2F20%3A10421617" target="_blank" >RIV/00216208:11320/20:10421617 - isvavai.cz</a>

  • Výsledek na webu

    <a href="https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=8GqxBqABfO" target="_blank" >https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=8GqxBqABfO</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1029/2019.11;018433" target="_blank" >10.1029/2019.11;018433</a>

Alternativní jazyky

  • Jazyk výsledku

    angličtina

  • Název v původním jazyce

    Reference Models for Lithospheric Geoneutrino Signal

  • Popis výsledku v původním jazyce

    Debate continues on the amount and distribution of radioactive heat producing elements (i.e., U, Th, and K) in the Earth, with estimates for mantle heat production varying by an order of magnitude. Constraints on the bulk-silicate Earth&apos;s (BSE) radiogenic power also places constraints on overall BSE composition. Geoneutrino detection is a direct measure of the Earth&apos;s decay rate of Th and U. The geoneutrino signal has contributions from the local (similar to 40%) and global (similar to 35%) continental lithosphere and the underlying inaccessible mantle (similar to 25%). Geophysical models are combined with geochemical data sets to predict the geoneutrino signal at current and future geoneutrino detectors. We propagated uncertainties, both chemical and physical, through Monte Carlo methods. Estimated total signal uncertainties are on the order of similar to 20%, proportionally with geophysical and geochemical inputs contributing similar to 30% and similar to 70%, respectively. We find that estimated signals, calculated using CRUST2.0, CRUST1.0, and LITHO1.0, are within physical uncertainty of each other, suggesting that the choice of underlying geophysical model will not change results significantly, but will shift the central value by up to similar to 15%. Similarly, we see no significant difference between calculated layer abundances and bulk crustal heat production when using these geophysical models. The bulk crustal heat production is calculated as 7 +/- 2 TW, which includes an increase of 1 TW in uncertainty relative to previous studies. Combination of our predicted lithospheric signal with measured signals yield an estimated BSE heat production of 21.5 +/- 10.4 TW. Future improvements, including uncertainty attribution and near-field modeling, are discussed.

  • Název v anglickém jazyce

    Reference Models for Lithospheric Geoneutrino Signal

  • Popis výsledku anglicky

    Debate continues on the amount and distribution of radioactive heat producing elements (i.e., U, Th, and K) in the Earth, with estimates for mantle heat production varying by an order of magnitude. Constraints on the bulk-silicate Earth&apos;s (BSE) radiogenic power also places constraints on overall BSE composition. Geoneutrino detection is a direct measure of the Earth&apos;s decay rate of Th and U. The geoneutrino signal has contributions from the local (similar to 40%) and global (similar to 35%) continental lithosphere and the underlying inaccessible mantle (similar to 25%). Geophysical models are combined with geochemical data sets to predict the geoneutrino signal at current and future geoneutrino detectors. We propagated uncertainties, both chemical and physical, through Monte Carlo methods. Estimated total signal uncertainties are on the order of similar to 20%, proportionally with geophysical and geochemical inputs contributing similar to 30% and similar to 70%, respectively. We find that estimated signals, calculated using CRUST2.0, CRUST1.0, and LITHO1.0, are within physical uncertainty of each other, suggesting that the choice of underlying geophysical model will not change results significantly, but will shift the central value by up to similar to 15%. Similarly, we see no significant difference between calculated layer abundances and bulk crustal heat production when using these geophysical models. The bulk crustal heat production is calculated as 7 +/- 2 TW, which includes an increase of 1 TW in uncertainty relative to previous studies. Combination of our predicted lithospheric signal with measured signals yield an estimated BSE heat production of 21.5 +/- 10.4 TW. Future improvements, including uncertainty attribution and near-field modeling, are discussed.

Klasifikace

  • Druh

    J<sub>imp</sub> - Článek v periodiku v databázi Web of Science

  • CEP obor

  • OECD FORD obor

    10500 - Earth and related environmental sciences

Návaznosti výsledku

  • Projekt

    <a href="/cs/project/GA17-01464S" target="_blank" >GA17-01464S: Studium radiogenního zahřívání Země metodami částicové geofyziky: geoneutrina a vzácné plyny</a><br>

  • Návaznosti

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

Ostatní

  • Rok uplatnění

    2020

  • Kód důvěrnosti údajů

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Údaje specifické pro druh výsledku

  • Název periodika

    Journal of Geophysical Research: Solid Earth

  • ISSN

    2169-9313

  • e-ISSN

  • Svazek periodika

    125

  • Číslo periodika v rámci svazku

    2

  • Stát vydavatele periodika

    US - Spojené státy americké

  • Počet stran výsledku

    17

  • Strana od-do

    e2019JB018433

  • Kód UT WoS článku

    000530895200054

  • EID výsledku v databázi Scopus