content_image/346906.jpg content_image/346904.jpg content_image/346903.jpg content_image/346900.jpg
nonzero moments for the second fragment Q (2) 0 = Z$_{2}$$_{/}$√$_{4}$$_{π}$ and Q (2) 2 = 3 Z 2 R 2 2 4 π β ∗ 2 $_{µ}$. Thus, we can write the expicit expressions for the dipole and quadrupole moment of the DNS in the form 

for the dipole moment and 

for the quadrupole moment. 

## D. Reduced transition probabilities 

<img src='content_image/346906.jpg'>

<img src='content_image/346904.jpg'>

Using expression (8) for the wave function and (19) for the multipole operators we can calculate the reduced transition probabilities as the 

<img src='content_image/346903.jpg'>

The reduced matrix elements for the multipole operator Q$_{λ}$ between the initial state i and the final state j has the following form 

<img src='content_image/346900.jpg'>

− { } { } (final) states. 

Using the two-level solutions for the ground-state band and the first excited negative par- ity bands we can easily calculate the explicit expression for the intraband B ( E 2) transitions and for the B ( E 1) transitions between these bands. 

