Within the special theory of relativity, the half life period of a particle measured in the laboratory frame is connected with its half life period measured in a frame moving with the particle as follows:
For both measurements we obtain:
"\\Rightarrow \\, \\Delta t_2 = \\frac{\\gamma_2}{\\gamma_1} \\Delta t_1"
Substituting the numerical values, we obtain:
Answer: 3 x 10-8 s.
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