(DSG ) (P ) (S ) (T ) (G ) (H ) (E ) (F ) (Ox ) (Oz ) (Cx ) (Cz ) (Tx ) (Tz ) (Lx ) (Lz )
Multipoles can be changed in magnitude by millifermis and the effect shown on a plot of the observable. The phase is kept fixed to avoid a violation of Watson's theorem, where valid. To select a multipole and its change, use the following notation: MJL: M = 1 for E(I=3/2) J = 1 for J=L-1/2 L = angular momentum 2 for M(I=3/2) 2 for J=L+1/2 of outgoing pi-N 3 for pE(I=1/2) 4 for pM(I=1/2) 5 for nE(I=1/2) 6 for nM(I=1/2) Example: The dominant M1 multipole (I=3/2) is MJL = 221 o Results are colour coded for changes of a positive or negative sign o Data references may be found using the "Observables" page o The conversion between millifermis and 10**(-3)/m_pi is: 197.33 MeV fm / 139.57 MeV ( or approximately sqrt(2) )