Branching ratio

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Many nuclides have more than one decay mode. Consider a nuclide in which there are two decay modes. The probability that an atom will decay by process 1 in time dt is k_1dt. Similarly the probability that it will decay by process 2 in time dt is k_2dt. Hence the equation governing the radioactive decay can be written as

dN/dt = �(k_1 + k_2)N

The total decay constant for the decay of the parent nuclide is k = k_1 + k_2. Hence, the branching ratios for modes 1 and 2 are defined as

BR_1 = k_1/k, BR_2 =k_2/k

In general, the branching ratio (BR) for a particular decay mode is defined as the ratio of the number of atoms decaying by that decay mode to the number decaying in total, i.e.

BR_i =k_i/(k_1 + k_2 + . . . k_i + . . .) = k_i/k

Alternatively, given the total decay constant, the “partial” decay constant is given by

k_i = BR_i · k

The relation between the decay constant and the half-life is given by

\tau = ln2/k0.693/k

and similar relations exist for the partial decay constant and the partial half-life, i.e.

\tau_i = ln2/k_i0.693/k_i = \tau/{BR}_i

where the subscript i refers to the particular mode of decay.


For the nuclide Ra-226, what is the partial half-life cluster decay?

The half-life of Ra-226 is 1600 y. The branching ratio for cluster decay is 2.6x10-11.

It follows that the partial half-life for cluster decay is (1600 y) / 2.6x10-11 = 6.15x1013 y


See half-life

Wikipedia on Branching Ratio

J. Magill and J. Galy, Radioactivity Radionuclides Radiation, Springer Verlag, 2005.

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