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Abstract
The proton light yield of liquid scintillators is an important property in the context of their use in large-scale neutrino experiments, with direct implications for neutrino-proton scattering measurements and the discrimination of fast neutrons from inverse
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1 University of California at Berkeley, Physics Department, Berkeley, USA (GRID:grid.47840.3f) (ISNI:0000 0001 2181 7878); Lawrence Berkeley National Laboratory, Nuclear Science Division, Berkeley, USA (GRID:grid.184769.5) (ISNI:0000 0001 2231 4551)
2 Lawrence Berkeley National Laboratory, Nuclear Science Division, Berkeley, USA (GRID:grid.184769.5) (ISNI:0000 0001 2231 4551); University of California at Berkeley, Department of Nuclear Engineering, Berkeley, USA (GRID:grid.47840.3f) (ISNI:0000 0001 2181 7878)
3 University of California at Berkeley, Department of Nuclear Engineering, Berkeley, USA (GRID:grid.47840.3f) (ISNI:0000 0001 2181 7878)
4 University of California at Berkeley, Department of Nuclear Engineering, Berkeley, USA (GRID:grid.47840.3f) (ISNI:0000 0001 2181 7878); Air Force Institute of Technology, Department of Engineering Physics, Wright-Patterson Air Force Base, USA (GRID:grid.427848.5) (ISNI:0000 0004 0614 1306)
5 Brookhaven National Laboratory, Chemistry Division, Upton, USA (GRID:grid.202665.5) (ISNI:0000 0001 2188 4229)