Knowledge of the bulk Lorentz factor Γ0 of GRBs allows us to
compute their comoving frame properties shedding light on their physics. Upon
collisions with the circumburst matter, the fireball of a GRB starts to
decelerate, producing a peak or a break (depending on the circumburst density
profile) in the light curve of the afterglow. Considering all bursts with known
redshift and with an early coverage of their emission, we find 67 GRBs with a
peak in their optical or GeV light curves at a time tp. For another
106 GRBs we set an upper limit tpUL. We show that tp
is due to the dynamics of the fireball deceleration and not to the passage of a
characteristic frequency of the synchrotron spectrum across the optical band.
Considering the tp of 66 long GRBs and the 85 most constraining upper
limits, using censored data analysis methods, we reconstruct the most likely
distribution of tp. All tp are larger than the time tp,g when the prompt emission peaks, and are much larger than the time tph when the fireball becomes transparent. The reconstructed distribution of
Γ0 has median value ∼300 (150) for a uniform (wind) circumburst
density profile. In the comoving frame, long GRBs have typical isotropic
energy, luminosity, and peak energy ⟨Eiso⟩=3(8)×1050 erg, ⟨Liso⟩=3(15)×1047 erg s−1 ,
and ⟨Epeak⟩=1(2) keV in the homogeneous (wind) case. We
confirm that the significant correlations between Γ and the rest frame
isotropic energy (Eiso), luminosity (Liso) and peak energy
(Epeak) are not due to selection effects. Assuming a typical opening
angle of 5 degrees, we derive the distribution of the jet baryon loading which
is centered around a few 10−6M⊙.Comment: 19 pages, 11 figures, 6 tables. Accepted for publication on Astronomy
& Astrophysic