For a closed unit-branching radioactive decay chain, the rate equations are
The first gives . Multiply the second by its integrating factor :
Integrate from zero to . For ,
so
The coefficients can individually be negative; the physical population is nonnegative because the production integral is nonnegative. For equal nuclear decay constants , the finite limit is
A sum of two constant-coefficient copies of the same exponential function cannot represent this limit; the factor is essential.

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