We consider the space-time metric generated by a global monopole in an extension of General Relativity (GR) of the form f (R) = R − λR 2 . The theory is formulated in the metric-affine (or Palatini) formalism and exact analytical solutions are obtained. For λ < 0, one finds that the solution has the same characteristics as the Schwarzschild black hole with a monopole charge in Einstein's GR. For λ > 0, instead, the metric is more closely related to the Reissner-Nordström metric with a monopole charge and, in addition, it possesses a wormhole-like structure that allows for the geodesic completeness of the space-time. Our solution recovers the expected limits when λ = 0 and also at the asymptotic far limit. The angular deflection of light in this spacetime in the weak field regime is also calculated. *