2018
DOI: 10.1016/j.matchar.2018.09.030
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Materials science applications of Neutron Depth Profiling at the PGAA facility of Heinz Maier-Leibnitz Zentrum

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Cited by 22 publications
(44 citation statements)
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“…All signals are cut at a depth of about 5.7 mg•cm −2 , which is the maximum depth limit for detection of 3 H charged particles in this setup. The inflection point, which resembles the anode-Cu current collector interphase [29], is situated around 6.0 ± 0.7 mg•cm −2 and lies outside of the detection range. In the bulk regime (0.5-3 mg•cm −2 ), a homogenous Li distribution was observed, indicating a homogenous distribution of the SEI.…”
Section: Sei Growth Phenomenamentioning
confidence: 88%
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“…All signals are cut at a depth of about 5.7 mg•cm −2 , which is the maximum depth limit for detection of 3 H charged particles in this setup. The inflection point, which resembles the anode-Cu current collector interphase [29], is situated around 6.0 ± 0.7 mg•cm −2 and lies outside of the detection range. In the bulk regime (0.5-3 mg•cm −2 ), a homogenous Li distribution was observed, indicating a homogenous distribution of the SEI.…”
Section: Sei Growth Phenomenamentioning
confidence: 88%
“…All depth profiles reveal a similar shape. An increase of lithium is detected at the anode surface, i.e., the anode-separator interphase, which might arise from surface orientation aspects or from direct lithium accumulations [29]. In deeper anode regions (>3 mg•cm −2 ) the signal decreased, resembling the Gaussian shape of the NDP detection response function.…”
Section: Sei Growth Phenomenamentioning
confidence: 91%
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