Processing math: 100%

 

 

 

Electromagnetic multipole moments and transitions

where we have defined la||[Yλ1(ˆr)l]λ||lb=(1)λ+la+lb(2λ+1)lb(lb+1)(2lb+1) ×{λ11λlblalb}la||Yλ1(ˆr)||lb, with la||Yλ1(ˆr)||lb=(1)la(2la+1)(2lb+1)(2λ1)4π(laλ1lb000).