Bibcode
Rodighiero, G.; Cimatti, A.; Gruppioni, C.; Popesso, P.; Andreani, P.; Altieri, B.; Aussel, H.; Berta, S.; Bongiovanni, A.; Brisbin, D.; Cava, A.; Cepa, J.; Daddi, E.; Dominguez-Sanchez, H.; Elbaz, D.; Fontana, A.; Förster Schreiber, N.; Franceschini, A.; Genzel, R.; Grazian, A.; Lutz, D.; Magdis, G.; Magliocchetti, M.; Magnelli, B.; Maiolino, R.; Mancini, C.; Nordon, R.; Perez Garcia, A. M.; Poglitsch, A.; Santini, P.; Sanchez-Portal, M.; Pozzi, F.; Riguccini, L.; Saintonge, A.; Shao, L.; Sturm, E.; Tacconi, L.; Valtchanov, I.; Wetzstein, M.; Wieprecht, E.
Referencia bibliográfica
Astronomy and Astrophysics, Volume 518, id.L25
Fecha de publicación:
7
2010
Revista
Número de citas
228
Número de citas referidas
220
Descripción
Aims: We exploit deep observations of the GOODS-N field taken
with PACS, the Photodetector Array Camera and Spectrometer, onboard of
Herschel, as part of the PACS evolutionary probe guaranteed time (PEP),
to study the link between star formation and stellar mass in galaxies to
z ~ 2. Methods: Starting from a stellar mass - selected sample of
~4500 galaxies with mag4.5 µm < 23.0 (AB), we
identify ~350 objects with a PACS detection at 100 or 160 μm and
~1500 with only Spitzer 24 μm counterpart. Stellar masses and total
IR luminosities (LIR) are estimated by fitting the spectral
energy distributions (SEDs). Results: Consistently with other
Herschel results, we find that LIR based only on 24 μm
data is overestimated by a median factor ~1.8 at z ~ 2, whereas it is
underestimated (with our approach) up to a factor ~1.6 at 0.5 < z
< 1.0. We then exploit this calibration to correct LIR
based on the MIPS/Spitzer fluxes. These results clearly show how
Herschel is fundamental to constrain LIR, and hence the star
formation rate (SFR), of high redshift galaxies. Using the galaxies
detected with PACS (and/or MIPS), we investigate the existence and
evolution of the relations between the SFR, the specific star formation
rate (SSFR=SFR/mass) and the stellar mass. Moreover, in order to avoid
selection effects, we also repeat this study through a stacking analysis
on the PACS images to fully exploit the far-IR information also for the
Herschel and Spitzer undetected subsamples. We find that the SSFR-mass
relation steepens with redshift, being almost flat at z < 1.0 and
reaching a slope of α = -0.50+0.13-0.16 at z
~ 2, at odds with recent works based on radio-stacking analysis at the
same redshift. The mean SSFR of galaxies increases with redshift, by a
factor ~15 for massive M > 1011 M&sun; galaxies
from z = 0 to z = 2, and seems to flatten at z > 1.5 in this mass
range. Moreover, the most massive galaxies have the lowest SSFR at any
z, implying that they have formed their stars earlier and more rapidly
than their low mass counterparts (downsizing).
Herschel is an ESA space observatory with science instruments provided
by European-led Principal Investigator consortia and with important
participation from NASA.Appendices are only available in electronic form
at http://www.aanda.org