Evolutionary status of dense cores in the NGC?1333 IRAS?4 star-forming region

摘要

Context. Protostellar evolution after the formation of the protostar is becoming reasonably well characterized, but the evolution from a prestellar core to a protostar is not well known, although the first hydrostatic core (FHSC) must be a pivotal step. Aims. NGC 1333 – IRAS 4C is a potentially very young object that we can directly compare with the nearby Class 0 objects IRAS 4A and IRAS 4B. Observational constraints are provided by spectral imaging from the JCMT Spectral Legacy Survey (330 ? 373 GHz). We present integrated intensity and velocity maps of several species, including CO, H _(2) CO and CH _(3) OH. CARMA observations provide additional information with which we can distinguish IRAS 4C from other evolutionary stages. Methods. We present the observational signatures of the velocity of an observed outflow, the degree of CO depletion, the deuterium fractionation of [DCO ~(+) ]/[HCO ~(+) ], and gas kinetic temperatures. Results. We report differences between the three sources in four aspects: a) the kinetic temperature as probed using the H _(2) CO lines is much lower toward IRAS 4C than the other two sources; b) the line profiles of the detected species show strong outflow activity toward IRAS 4A and IRAS 4B, but not toward IRAS 4C; c) the HCN/HNC is & 1 toward IRAS 4C, which confirms the cold nature of the source; d) the degree of CO depletion and the deuteration are lowest toward the warmest of the sources, IRAS 4B. Conclusions. IRAS 4C seems to be in a different evolutionary state than the sources IRAS 4A and IRAS 4B. We can probably exclude the FHSC stage becaues of the relatively low L _(smm) / L _(bol) ( ~ 6%), and we investigate the earliest accretion phase of Class 0 stage and the transition between Class 0 to Class I. Our results do not show a consistent scenario for either case; the main problem is the absence of outflow activity and the cold nature of IRAS 4C. The number of FHSC candidates in Perseus is ~ 10 times higher than current models predict, which suggests that the lifespan of these objects is ≥ 10 ~(3) yrs, which might be due to an accretion rate lower than 4 × 10 ~(-5) M _(⊙) /yr.