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In a coalescence plus independent fragmentation approach we calculate the$p_T$ spectra of the main hadrons: $\pi, K, p, \bar p, \Lambda, \phi$ in a widerange of transverse momentum from low $p_T$ up to about 10 GeV. The approach inits main features was developed several years ago at RHIC energy. Augmentingthe model with the inclusion of some more main resonance decays, we show thatthe approach correctly predicts the evolution of the $p_T$ spectra from RHIC toLHC energy and in particular the baryon-to-meson ratios $p/\pi,\barp/\pi,\Lambda/K$ that reach a value of the order of unit at $p_T \sim 3\, \rmGeV$. This is achieved without any change of the coalescence parameters. Themore recent availability of experimental data up to $p_T \sim 10\rm\, GeV$ for$\Lambda$ spectrum as well as for $p/\pi$ and $\Lambda/K$ shows some lack ofyield in a limited $p_T$ range around 6 GeV. This indicates that the baryons$p_T$ spectra from AKK fragmentation functions are too flat at $p_T\lesssim 8\,\rm GeV$. We also show that in a coalescence plus fragmentation approach onepredicts a nearly $p_T$ independent $p/\phi$ ratio up to $p_T \sim 4 \rm\, GeV$followed by a significant decrease at higher $p_T$. Such a behavior is drivenby a similar radial flow effect at $p_T< 2 \,\rm GeV$ and the dominance offragmentation for $\phi$ at larger $p_T$.

Hadrons from Coalescence plus Fragmentation in AA collisions from RHIC to LHC energy