Yields and production rates of cosmogenic $^9$Li and $^8$He measured with the Double Chooz near and far detectors
H. de Kerret, T. Abrah\~ao, H. Almazan, J.C. dos Anjos, S. Appel, J.C., Barriere, I. Bekman, T.J.C. Bezerra, L. Bezrukov, E. Blucher, T. Brugi\`ere,, C. Buck, J. Busenitz, A. Cabrera, M. Cerrada, E. Chauveau, P. Chimenti, O., Corpace, J.V. Dawson, Z. Djurcic, A. Etenko

TL;DR
This study measures the production rates of cosmogenic isotopes $^9$Li and $^8$He at two different detector sites, establishing a relationship between $^9$Li yield and muon energy to aid future background predictions.
Contribution
It provides the first multi-experiment, data-driven relationship between $^9$Li yield and muon energy based on measurements at different depths.
Findings
$^8$He contribution is compatible with zero.
Measured $^9$Li yields are 5.51 and 7.90 in units of 10^{-8}μ^{-1} g^{-1}cm^{2}.
Established a power-law relationship between $^9$Li yield and muon energy.
Abstract
The yields and production rates of the radioisotopes Li and He created by cosmic muon spallation on C, have been measured by the two detectors of the Double Chooz experiment. The identical detectors are located at separate sites and depths, which means they are subject to different muon spectra. The near (far) detector has an overburden of 120 m.w.e. (300 m.w.e.) corresponding to a mean muon energy of (). Comparing the data to a detailed simulation of the Li and He decays, the contribution of the He radioisotope at both detectors is found to be compatible with zero. The observed Li yields in the near and far detectors are and , respectively, in units of . The shallow overburdens of the near and far detectors give a unique…
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