5 Eki ki

The accelerated particle spectrum at 3 = 1/2 will be found, using the distribution described by Eq. 4.2.7 over the times of particle t acceleration in the source and the dependence of the mean lifetime t on Ek (see Eq. 4.5.4). The spectrum found of the accelerated particles may be presented in the form of Eq. 4.2.9, i.e. n(Ek)— E_Y, but with a variable power exponent

Y = 2 + 3AiEk/ 8ufTiy[2maajEi In the moderate-energy range

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