The decay rate \( R(t) \) of a radioactive sample is given by the equation: \[ R(t) = R_0 e^{-\lambda t} \] where \( R_0 \) is the initial decay rate, \( \lambda \) is the decay constant, and \( t \) is the time. After one half-life \( T_{1/2} \), the decay rate is reduced by half.
Therefore, the decay rate after half-life is: \[ R(T_{1/2}) = \frac{R_0}{2} \] Thus, after one half-life, the decay rate of the sample is \( \frac{R_0}{2} \).