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Deuterium is the most fragile of the light nuclei and the most informative. The scan gives a logarithmic sensitivity of 0.15 for the deuterium abundance with respect to the bounce temperature in the range examined. A bounce at 0.2 MeV would leave a residue of 2.16e-05, well below the observed value, while a bounce at 1 MeV leaves 2.52e-05, close to the standard 2.53e-05. Deuterium therefore excludes a low bounce more firmly, per unit of observational effort, than any other single light element considered in isolation. Computed from stated assumptions, not measured.
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William Alexander Aldred (2026) studied this question.
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