Article,

A description of the f2(1270), rho3(1690), f4(2050), rho5(2350) and f6(2510) resonances as multi-rho(770) states

, and .
(May 3, 2010)

Abstract

In a previous work regarding the interaction of two \$\rho(770)\$ resonances, the \$f\_2(1270)\$ (\$J^PC=2^++\$) resonance was obtained dynamically as a two-\$\rho\$ molecule with a very strong binding energy, 135\~MeV per \$\rho\$ particle. In the present work we use the \$\rho\rho\$ interaction in spin 2 and isospin 0 channel to show that the resonances \$\rho\_3(1690)\$ (\$3^--\$), \$f\_4(2050)\$ (\$4^++\$), \$\rho\_5(2350)\$ (\$5^--\$) and \$f\_6(2510)\$ (\$6^++\$) are basically molecules of increasing number of \$\rho(770)\$ particles. We use the fixed center approximation of the Faddeev equations to write the multi-body interaction in terms of the two-body scattering amplitudes. We find the masses of the states very close to the experimental values and we get an increasing value of the binding energy per \$\rho\$ as the number of \$\rho\$ mesons is increased.

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