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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