content_image/358716.jpg content_image/358717.jpg content_image/358715.jpg content_image/358714.jpg content_image/358713.jpg content_image/358712.jpg
where 

with the energy is given as 

Angular momentum I can take only odd values. 

## C. Multipole Moments 

Electric multipole operators are given by the expression 

For the dinuclear system we assume that 

<img src='content_image/358716.jpg'>

<img src='content_image/358717.jpg'>

<img src='content_image/358715.jpg'>

<img src='content_image/358714.jpg'>

where ρ$_{i}$ ( i = 1 , 2) are the densities of the DNS fragments. Using (18) we can rewrite the expression for the electric multipole moments for the DNS in the following form 

<img src='content_image/358713.jpg'>

where 

<img src='content_image/358712.jpg'>

In the last expression Q ( i ) ( i = 1 , 2) are the intrinsic multipole moments of the DNS frag- ments. 

Since we assume that the light fragment is spherical and can not be excited in the con- sidered energy range the only nonzero moment for the first fragment is Q (1) 0 = Z$_{1}$$_{/}$√$_{4}$$_{π}$$_{.}$ The second fragment is assumed to perform the quadrupole oscillations around the spheri- cal shape. Thus, in the linear approximation with respect to the deformation, we have two 

