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Nuclear, Atomic Physics Governing Changes in Relativistic

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1) -1 \>. L (55) ) l=il (K) and where il(K) denotes the first isotope belonging to the element in and in(K) denotes the last isotope. the K""th row of1-l points about isotope ~ . First, as shown in Eq. (55), the collapse to element was done by weighting fractions at the source. Note two Secondly, from M-l with the assumed isotope multiplying Eq. (54) by vi! gives the equation (56) ~ = -A v1;j ~ is in which completely specified in terms of the input quantities and the parameters. Because so many --6f the terms of M and product of a cross section and the parameter for display purposes to give the matrices section.

Intermediate propagated. reaction interstellar links cross section with line that, but by the The notation' attachment As discussed Note also Lastly, these cross sections half-life, but sometimes by electron for decay by this mode followed more often as in the In these capture. one electron earlier, 'a/EC" in ) CT1 ~, EC attached "clock" isotopes case of 60pe, decay short- in a decay chain do not have to be explicitly 2 of the figure gives the total per hydrogen atom. include an estimate helium and were calculated As discussed effective in § II(d), of the contributions using a slight of Karol's analytic version of the Glauber fonnalism.

MlHlich), 12, 4183.

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