  We review how Quark-Hadron Duality (QHD) for (u,d) flavors at high energies
and in the scaling regime suggests a radial and angular behaviour of mesonic
and baryonic resonance masses of the Regge form $M^2_{nJ} = \mu^2 n + \beta^2 J
+ M_0^2 $. The radial mass dependence is asymptotically consistent with a
common two-body dynamics for mesons and baryons in terms of the quark-antiquark
($q \bar q)$ and quark-diquark ($qD$) degrees of freedom, respectively. This
formula is validated phenomenologically within an uncertainty determined by
half the width of the resonances, $\Delta M_{nJ}^2 \sim \Gamma_{nJ} M_{nJ}$.
With this error prescription we find from the non-strange PDG hadrons different
radial slopes $\mu^2_{\bar qq}=1.34(4) {\rm GeV}^2$ and $\mu^2_{qD}=0.75(3)
{\rm GeV}^2$, but similar angular slopes $\beta_{\bar q q}^2 \sim \beta_{ q
D}^2 \sim 1.15 {\rm GeV}^2$.
