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Table 3

SNR evolution when SNR evolving into the MS bubble shell.

Scenariosa R b,MS E ej M ej R SNR, end t SNR, end v SNR, end n end b η esc E max, end E CR,end E CR,sh c

20M in-shell 20.5 pc 2 E51 2 M 15 pc 4.9 kyr 1150 km s-1 0.58 cm-3 0.02 15.6 TeV 0.13 E51 0.12 E51
25M in-shell 21.5 pc 2 E51 2 M 15 pc 2.4 kyr 1170 km s-1 0.35 cm-3 0.02 6.6 TeV 0.08 E51 0.07 E51

Notes.

(a)

For both scenarios, the same initial progenitor star (scenario 20 M, SNe IIL/b and scenario 25 M, SNe Ib/c) and the same RSG bubble structure as shown in Table 1 are assumed. They only differ in MS bubble shell structure and SN energy.

(b)

The gas density in the upstream of the shock at tSNR, end.

(c)

The total CR energy trapped inside the downstream of the shock at tSNR, end. Here we roughly assume that the total CR number .

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