No.

E1 transitions

Comments

No.

M1 transitions

Comments

1

As the GS is matched with the ⁶Р_3/2 level, it is possible to consider E1 transitions from the ⁶S_5/2 scattering wave to the GS of ¹¹B.

6

Furthermore, it is possible to consider M1 transitions to the GS from the resonance scattering wave ⁶Р_5/2 at 0.475(17) MeV, and from the non-resonance ⁶Р_3/2 wave. As will be shown later, the cross section of the transition for the first variant of the ⁶Р_3/2 scattering potential with zero depth will stay at the level 1 - 2 μb, and the other transitions from the non-resonance waves will not be considered.

2

In addition, it is possible to consider E1 transitions from the ⁶S_5/2 and ⁸S_7/2 scattering waves to the second ES of ¹¹B, which is the mixture of two P states. Because here we have transitions from the initial S states that differ by spin to the different parts of one total WF of the BS, the cross section of these transitions will sum up, i.e.,.

7

Furthermore, it is possible to consider M1 transitions to the second ES ⁶P_5/2 and ⁸P_5/2 from the resonance ⁶P_5/2 and ⁸P_5/2 scattering waves. Because this is the transition from the mixed-by-spin Р_5/2 scattering wave to the mixed-by-spin second ES, the cross section will be averaged according to transitions given above, i.e.,.

3

The third ES is matched with the ⁶Р_3/2 level as the GS, and it is possible to consider the E1 transitions from the ⁵S_5/2 scattering waves to this ES of ¹¹B.

8

It is possible to consider the M1 transitions to the third ES ⁶P_3/2 from the resonance ⁶Р_5/2 scattering wave.

4

Another E1 transition is possible from the ⁶S_5/2 and ⁸S_7/2 scattering waves of the fourth ES of ¹¹B at. The cross section of these two transitions will also sum up.

9

The M1 transitions are feasible to the fourth ES from the resonance scattering wave. This cross section will be averaged over two transitions, as was given in the case of reaction 7.

5

The last of considered E1 transitions is the capture from the ⁶S_5/2 and ⁸S_7/2 scattering waves to the ninth ES of ¹¹B at. The cross section of these transitions will also sum up, as given in the case of reaction 2.

10

Finally, we can consider the M1 transitions to the ninth ES from the resonance scattering wave, because there are experimental data of [60] for this. This cross section will also be averaged over the two transitions to the ES given here.