Ab initio electronic stopping power for protons in Ga0.5In0.5P/GaAs/Ge triple-junction solar cells for space applications
Data files
Oct 20, 2020 version files 21.38 MB
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Etot-z-GaAs96-linear-fit-channel001-traj1.pdf
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Etot-z-GaAs96-linear-fit-channel001-traj2.pdf
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Etot-z-GaAs96-linear-fit-channel001-traj3.pdf
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Etot-z-GaAs96-linear-fit-channel011-traj1.pdf
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Etot-z-GaAs96-linear-fit-channel011-traj2.pdf
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Etot-z-GaAs96-linear-fit-channel011-traj3.pdf
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Etot-z-GaAs96-linear-fit-channel011-traj4.pdf
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Etot-z-GaInP2-linear-fit-channel001-traj1.pdf
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Etot-z-GaInP2-linear-fit-channel001-traj2.pdf
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Etot-z-GaInP2-linear-fit-channel001-traj3.pdf
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Etot-z-GaInP2-linear-fit-channel001-traj4.pdf
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Etot-z-GaInP2-linear-fit-channel011-traj1.pdf
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Etot-z-GaInP2-linear-fit-channel011-traj2.pdf
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Etot-z-GaInP2-linear-fit-channel011-traj3.pdf
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Etot-z-GaInP2-linear-fit-channel011-traj4.pdf
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Etot-z-Ge96-linear-fit-channel001-traj1.pdf
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Etot-z-Ge96-linear-fit-channel001-traj2.pdf
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Etot-z-Ge96-linear-fit-channel001-traj3.pdf
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Etot-z-Ge96-linear-fit-channel011-traj1.pdf
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Etot-z-Ge96-linear-fit-channel011-traj2.pdf
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Etot-z-Ge96-linear-fit-channel011-traj3.pdf
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Etot-z-Ge96-linear-fit-channel011-traj4.pdf
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Etot-z-Ge96-linear-fit-channel011-traj5.pdf
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fdf-GaAs-192.log
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fdf-GaAs-96.log
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fdf-GaInP2-192.log
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fdf-GaInP2-96.log
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fdf-GaInP2-GaAs-interface.log
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fdf-Ge-96.log
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GaAs-channel001-traj1-v-0_2.TDETOT
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GaAs-channel001-traj1-v-0_3.TDETOT
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GaAs-channel001-traj1-v-0_4.TDETOT
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GaAs-channel001-traj1-v-0_5.TDETOT
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GaAs-channel001-traj1-v-0_6.TDETOT
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GaAs-channel001-traj1-v-0_7.TDETOT
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GaAs-channel001-traj1-v-0_8.TDETOT
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GaAs-channel001-traj1-v-0_9.TDETOT
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GaAs-channel001-traj2-v-0_2.TDETOT
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GaAs-channel001-traj2-v-0_3.TDETOT
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GaAs-channel001-traj2-v-0_4.TDETOT
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GaAs-channel001-traj2-v-0_5.TDETOT
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GaAs-channel001-traj2-v-0_6.TDETOT
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GaAs-channel001-traj2-v-0_7.TDETOT
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GaAs-channel001-traj2-v-0_8.TDETOT
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GaAs-channel001-traj2-v-0_9.TDETOT
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GaAs-channel001-traj3-v-0_2.TDETOT
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GaAs-channel001-traj3-v-0_3.TDETOT
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GaAs-channel001-traj3-v-0_4.TDETOT
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GaAs-channel001-traj3-v-0_5.TDETOT
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GaAs-channel001-traj3-v-0_6.TDETOT
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GaAs-channel001-traj3-v-0_7.TDETOT
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GaAs-channel001-traj3-v-0_8.TDETOT
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GaAs-channel001-traj3-v-0_9.TDETOT
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GaAs-channel011-traj1-v-0_2.TDETOT
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GaAs-channel011-traj1-v-0_3.TDETOT
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GaAs-channel011-traj1-v-0_4.TDETOT
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GaAs-channel011-traj1-v-0_5.TDETOT
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GaAs-channel011-traj1-v-0_6.TDETOT
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GaAs-channel011-traj1-v-0_7.TDETOT
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GaAs-channel011-traj1-v-0_8.TDETOT
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GaAs-channel011-traj1-v-0_9.TDETOT
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GaAs-channel011-traj2-v-0_2.TDETOT
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GaAs-channel011-traj2-v-0_3.TDETOT
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GaAs-channel011-traj2-v-0_4.TDETOT
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GaAs-channel011-traj2-v-0_5.TDETOT
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GaAs-channel011-traj2-v-0_6.TDETOT
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GaAs-channel011-traj2-v-0_7.TDETOT
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GaAs-channel011-traj2-v-0_8.TDETOT
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GaAs-channel011-traj2-v-0_9.TDETOT
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GaAs-channel011-traj3-v-0_2.TDETOT
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GaAs-channel011-traj3-v-0_3.TDETOT
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GaAs-channel011-traj3-v-0_4.TDETOT
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GaAs-channel011-traj3-v-0_5.TDETOT
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GaAs-channel011-traj3-v-0_6.TDETOT
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GaAs-channel011-traj3-v-0_7.TDETOT
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GaAs-channel011-traj3-v-0_8.TDETOT
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GaAs-channel011-traj3-v-0_9.TDETOT
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GaAs-channel011-traj4-v-0_2.TDETOT
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GaAs-channel011-traj4-v-0_3.TDETOT
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GaAs-channel011-traj4-v-0_4.TDETOT
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GaAs-channel011-traj4-v-0_5.TDETOT
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GaAs-channel011-traj4-v-0_6.TDETOT
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GaAs-channel011-traj4-v-0_7.TDETOT
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GaAs-channel011-traj4-v-0_8.TDETOT
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GaAs-channel011-traj4-v-0_9.TDETOT
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GaAs192-channel-001-v-0_3.TDETOT
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GaAs192-channel-001-v-0_6.TDETOT
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GaAs192-off-center-channel-001-v-0_3.TDETOT
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GaAs192-off-center-channel-001-v-0_6.TDETOT
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GaInP-GaAs-int-channel-001-v-0_3.TDETOT
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GaInP-GaAs-int-channel-001-v-0_6.TDETOT
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GaInP-GaAs-int-off-center-channel-001-v-0_3.TDETOT
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GaInP-GaAs-int-off-center-channel-001-v-0_6.TDETOT
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GaInP2-192-channel-001-v-0_3.TDETOT
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GaInP2-192-channel-001-v-0_6.TDETOT
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GaInP2-192-off-center-channel-001-v-0_3.TDETOT
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GaInP2-192-off-center-channel-001-v-0_6.TDETOT
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GaInP2-channel001-traj1-v-0_2.TDETOT
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GaInP2-channel001-traj1-v-0_3.TDETOT
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GaInP2-channel001-traj1-v-0_4.TDETOT
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GaInP2-channel001-traj1-v-0_5.TDETOT
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GaInP2-channel001-traj1-v-0_6.TDETOT
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GaInP2-channel001-traj1-v-0_7.TDETOT
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GaInP2-channel001-traj1-v-0_8.TDETOT
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GaInP2-channel001-traj1-v-0_9.TDETOT
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GaInP2-channel001-traj2-v-0_2.TDETOT
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GaInP2-channel001-traj2-v-0_3.TDETOT
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GaInP2-channel001-traj2-v-0_4.TDETOT
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GaInP2-channel001-traj2-v-0_5.TDETOT
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GaInP2-channel001-traj2-v-0_6.TDETOT
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GaInP2-channel001-traj2-v-0_7.TDETOT
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GaInP2-channel001-traj2-v-0_8.TDETOT
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GaInP2-channel001-traj2-v-0_9.TDETOT
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GaInP2-channel001-traj3-v-0_2.TDETOT
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GaInP2-channel001-traj3-v-0_3.TDETOT
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GaInP2-channel001-traj3-v-0_4.TDETOT
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GaInP2-channel001-traj3-v-0_5.TDETOT
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GaInP2-channel001-traj3-v-0_6.TDETOT
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GaInP2-channel001-traj3-v-0_7.TDETOT
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GaInP2-channel001-traj3-v-0_8.TDETOT
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GaInP2-channel001-traj3-v-0_9.TDETOT
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GaInP2-channel001-traj4-v-0_2.TDETOT
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GaInP2-channel001-traj4-v-0_3.TDETOT
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GaInP2-channel001-traj4-v-0_4.TDETOT
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GaInP2-channel001-traj4-v-0_5.TDETOT
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GaInP2-channel001-traj4-v-0_6.TDETOT
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GaInP2-channel001-traj4-v-0_7.TDETOT
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GaInP2-channel001-traj4-v-0_8.TDETOT
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GaInP2-channel001-traj4-v-0_9.TDETOT
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GaInP2-channel011-traj1-v-0_2.TDETOT
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GaInP2-channel011-traj1-v-0_3.TDETOT
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GaInP2-channel011-traj1-v-0_4.TDETOT
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GaInP2-channel011-traj1-v-0_5.TDETOT
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GaInP2-channel011-traj1-v-0_6.TDETOT
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GaInP2-channel011-traj1-v-0_7.TDETOT
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GaInP2-channel011-traj1-v-0_8.TDETOT
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GaInP2-channel011-traj1-v-0_9.TDETOT
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GaInP2-channel011-traj2-v-0_2.TDETOT
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GaInP2-channel011-traj2-v-0_3.TDETOT
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GaInP2-channel011-traj2-v-0_4.TDETOT
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GaInP2-channel011-traj2-v-0_5.TDETOT
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GaInP2-channel011-traj2-v-0_6.TDETOT
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GaInP2-channel011-traj2-v-0_7.TDETOT
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GaInP2-channel011-traj2-v-0_8.TDETOT
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GaInP2-channel011-traj2-v-0_9.TDETOT
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GaInP2-channel011-traj3-v-0_2.TDETOT
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GaInP2-channel011-traj3-v-0_3.TDETOT
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GaInP2-channel011-traj3-v-0_4.TDETOT
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GaInP2-channel011-traj3-v-0_5.TDETOT
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GaInP2-channel011-traj3-v-0_6.TDETOT
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GaInP2-channel011-traj3-v-0_7.TDETOT
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GaInP2-channel011-traj3-v-0_8.TDETOT
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GaInP2-channel011-traj3-v-0_9.TDETOT
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GaInP2-channel011-traj4-v-0_2.TDETOT
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GaInP2-channel011-traj4-v-0_3.TDETOT
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GaInP2-channel011-traj4-v-0_4.TDETOT
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GaInP2-channel011-traj4-v-0_5.TDETOT
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GaInP2-channel011-traj4-v-0_6.TDETOT
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GaInP2-channel011-traj4-v-0_7.TDETOT
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GaInP2-channel011-traj4-v-0_8.TDETOT
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GaInP2-channel011-traj4-v-0_9.TDETOT
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Ge-channel001-traj1-v-0_2.TDETOT
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Ge-channel001-traj1-v-0_3.TDETOT
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Ge-channel001-traj1-v-0_4.TDETOT
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Ge-channel001-traj1-v-0_5.TDETOT
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Ge-channel001-traj1-v-0_6.TDETOT
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Ge-channel001-traj1-v-0_7.TDETOT
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Ge-channel001-traj1-v-0_8.TDETOT
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Ge-channel001-traj1-v-0_9.TDETOT
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Ge-channel001-traj2-v-0_2.TDETOT
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Ge-channel001-traj2-v-0_3.TDETOT
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Ge-channel001-traj2-v-0_4.TDETOT
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Ge-channel001-traj2-v-0_5.TDETOT
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Ge-channel001-traj2-v-0_6.TDETOT
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Ge-channel001-traj2-v-0_7.TDETOT
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Ge-channel001-traj2-v-0_8.TDETOT
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Ge-channel001-traj2-v-0_9.TDETOT
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Ge-channel001-traj3-v-0_2.TDETOT
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Ge-channel001-traj3-v-0_3.TDETOT
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Ge-channel001-traj3-v-0_4.TDETOT
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Ge-channel001-traj3-v-0_5.TDETOT
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Ge-channel001-traj3-v-0_6.TDETOT
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Ge-channel001-traj3-v-0_7.TDETOT
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Ge-channel001-traj3-v-0_8.TDETOT
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Ge-channel001-traj3-v-0_9.TDETOT
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Ge-channel011-traj1-v-0_2.TDETOT
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Ge-channel011-traj1-v-0_3.TDETOT
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Ge-channel011-traj1-v-0_4.TDETOT
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Ge-channel011-traj1-v-0_5.TDETOT
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Ge-channel011-traj1-v-0_6.TDETOT
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Ge-channel011-traj1-v-0_7.TDETOT
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Ge-channel011-traj1-v-0_8.TDETOT
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Ge-channel011-traj1-v-0_9.TDETOT
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Ge-channel011-traj2-v-0_2.TDETOT
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Ge-channel011-traj2-v-0_3.TDETOT
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Ge-channel011-traj2-v-0_4.TDETOT
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Ge-channel011-traj2-v-0_5.TDETOT
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Ge-channel011-traj2-v-0_6.TDETOT
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Ge-channel011-traj2-v-0_8.TDETOT
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Ge-channel011-traj2-v-0_9.TDETOT
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Ge-channel011-traj3-v-0_2.TDETOT
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Ge-channel011-traj3-v-0_3.TDETOT
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Ge-channel011-traj3-v-0_4.TDETOT
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Ge-channel011-traj3-v-0_5.TDETOT
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Ge-channel011-traj3-v-0_9.TDETOT
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Ge-channel011-traj4-v-0_2.TDETOT
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Ge-channel011-traj4-v-0_3.TDETOT
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Ge-channel011-traj4-v-0_4.TDETOT
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Ge-channel011-traj4-v-0_5.TDETOT
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Ge-channel011-traj4-v-0_9.TDETOT
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Ge-channel011-traj5-v-0_2.TDETOT
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NOTE
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stopping-vs-velocity-GaAs-channel001-traj1.dat
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stopping-vs-velocity-GaAs-channel001-traj2.dat
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stopping-vs-velocity-GaAs-channel001-traj3.dat
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stopping-vs-velocity-GaAs-channel011-traj1.dat
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stopping-vs-velocity-GaAs-channel011-traj2.dat
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stopping-vs-velocity-GaAs-channel011-traj3.dat
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stopping-vs-velocity-GaAs-channel011-traj4.dat
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stopping-vs-velocity-GaInP2-channel001-traj1.dat
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stopping-vs-velocity-GaInP2-channel001-traj2.dat
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stopping-vs-velocity-GaInP2-channel001-traj3.dat
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stopping-vs-velocity-GaInP2-channel001-traj4.dat
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stopping-vs-velocity-GaInP2-channel011-traj1.dat
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stopping-vs-velocity-GaInP2-channel011-traj2.dat
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stopping-vs-velocity-GaInP2-channel011-traj3.dat
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stopping-vs-velocity-GaInP2-channel011-traj4.dat
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stopping-vs-velocity-Ge-channel001-traj1.dat
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stopping-vs-velocity-Ge-channel001-traj2.dat
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stopping-vs-velocity-Ge-channel001-traj3.dat
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stopping-vs-velocity-Ge-channel011-traj1.dat
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stopping-vs-velocity-Ge-channel011-traj2.dat
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stopping-vs-velocity-Ge-channel011-traj3.dat
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stopping-vs-velocity-Ge-channel011-traj4.dat
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stopping-vs-velocity-Ge-channel011-traj5.dat
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Abstract
Motivated by the radiation damage of solar panels in space, firstly, the results of Monte Carlo particle transport simulations are presented for proton impact on triple-junction Ga0.5In0.5P/GaAs/Ge solar cells, showing the proton projectile penetration in the cells as a function of energy. It is followed by a systematic ab initio investigation of the electronic stopping power for protons in different layers of the cell at the relevant velocities via real-time time-dependent density functional theory (RT-TDDFT) calculations. The electronic stopping power is found to depend significantly on different channeling conditions, which should affect the low velocity damage predictions, and which are understood in terms of impact parameter and electron density along the path. Additionally, we explore the effect of the interface between the layers of the multilayer structure on the energy loss of a proton, along with the effect of strain in the lattice-matched solar cell. Both effects are found to be small compared with the main bulk effect. The interface energy loss has been found to increase with decreasing proton velocity, and in one case, there is an effective interface energy gain.