Graziano Coppa

Dr. Graziano Coppa

Istituto Nazionale di Ricerca Metrologica, 10135 Turin, Italy
orcid

Research Focus & Metrics

Academic Career Length

19Years (2008-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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26 August 2010 in The Astrophysical Journal
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YPYing-Jie Peng
Ying-Jie Peng
SLSimon J. Lilly
Simon J. Lilly
KKKatarina Kovač
Katarina Kovač
MBMicol Bolzonella
Micol Bolzonella
LPLucia Pozzetti
Lucia Pozzetti
RSRoberto Scaramella
Roberto Scaramella
We explore the inter-relationships between mass, star-formation rate and environment in the SDSS, zCOSMOS and other surveys. The differential effects of mass and environment are completely separable to z ~ 1, indicating that two distinct processes are operating, "mass-quenching" and "environment-quenching". Environment-quenching, at fixed over-density, evidently does not change with epoch to z ~ 1, suggesting that it occurs as large-scale structure develops in the Universe. The observed constancy of the mass-function shape for star-forming galaxies, demands that the mass-quenching of galaxies around and above M*, must be proportional to their star-formation rates at all z < 2. We postulate that this simple mass-quenching law also holds over a much broader range of stellar mass and epoch. These two simple quenching processes, plus some additional quenching due to merging, then naturally produce (a) a quasi-static Schechter mass function for star-forming galaxies with a value of M* that is set by the proportionality between the star-formation and mass-quenching rates, (b) a double Schechter function for passive galaxies with two components: the dominant one is produced by mass-quenching and has exactly the same M* as the star-forming galaxies but an alpha shallower by +1, while the other is produced by environment effects and has the same M* and alpha as the star-forming galaxies, and is larger in high density environments. Subsequent merging of quenched galaxies modifies these predictions somewhat in the denser environments, slightly increasing M* and making alpha more negative. All of these detailed quantitative relationships between the Schechter parameters are indeed seen in the SDSS, lending strong support to our simple empirically-based model. The model naturally produces for passive galaxies the "anti-hierarchical" run of mean ages and alpha-element abundances with mass.

1 August 2012 in Journal of Cosmology and Astroparticle Physics
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MMM. Moresco
M. Moresco
ACA. Cimatti
A. Cimatti
RJR. Jimenez
R. Jimenez
LPL. Pozzetti
L. Pozzetti
GZG. Zamorani
G. Zamorani
NWN. Welikala
N. Welikala
We present new improved constraints on the Hubble parameterH(z) in the redshift range 0.15 <z< 1.1, obtained from the differential spectroscopic evolution of early-type galaxies as a function of redshift. We extract a large sample of early-type galaxies ( ∼ 11000) from several spectroscopic surveys, spanning almost 8 billion years of cosmic lookback time (0.15 <z< 1.42). We select the most massive, red elliptical galaxies, passively evolving and without signature of ongoing star formation. Those galaxies can be used as standard cosmic chronometers, as firstly proposed by Jimenez & Loeb (2002), whose differential age evolution as a function of cosmic time directly probesH(z). We analyze the 4000 Å break (D4000) as a function of redshift, use stellar population synthesis models to theoretically calibrate the dependence of the differential age evolution on the differentialD4000, and estimate the Hubble parameter taking into account both statistical and systematical errors. We provide 8 new measurements ofH(z) (see table 4), and determine its change inH(z) to a precision of 5–12% mapping homogeneously the redshift range up toz∼ 1.1; for the first time, we place a constraint onH(z) atz≠0 with a precision comparable with the one achieved for the Hubble constant (about 5–6% atz∼ 0.2), and covered a redshift range (0.5 <z< 0.8) which is crucial to distinguish many different quintessence cosmologies. These measurements have been tested to best match a ΛCDM model, clearly providing a statistically robust indication that the Universe is undergoing an accelerated expansion. This method shows the potentiality to open a new avenue in constrain a variety of alternative cosmologies, especially when future surveys (e.g. Euclid) will open the possibility to extend it up toz∼ 2.

8 December 2008 in The Astrophysical Journal
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Journal Article
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OIO. Ilbert
O. Ilbert
PCP. Capak
P. Capak
MSM. Salvato
M. Salvato
HAH. Aussel
H. Aussel
HMH. J. McCracken
H. J. McCracken
EZE. Zucca
E. Zucca

15 September 2009 in The Astrophysical Journal Supplement Series
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SLSimon J. Lilly
Simon J. Lilly
VBVincent Le Brun
Vincent Le Brun
CMChristian Maier
Christian Maier
VMVincenzo Mainieri
Vincenzo Mainieri
MMMarco Mignoli
Marco Mignoli
YTYoshiaki Taniguchi
Yoshiaki Taniguchi

10 November 2010 in Astronomy & Astrophysics
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LPL. Pozzetti
L. Pozzetti
MBM. Bolzonella
M. Bolzonella
EZE. Zucca
E. Zucca
GZG. Zamorani
G. Zamorani
SLS. Lilly
S. Lilly
NSN. Scoville
N. Scoville
We present the galaxy stellar mass function (GSMF) to redshift z ≃ 1, based on the analysis of about 8500 galaxies with I < 22.5 (AB mag) over 1.4 deg2, which are part of the zCOSMOS-bright 10k spectroscopic sample. We investigate the total GSMF, as well as the contributions of early- and late-type galaxies (ETGs and LTGs, respectively), defined by different criteria (broad-band spectral energy distribution, morphology, spectral properties, or star formation activities). We unveil a galaxybimodality in the global GSMF, whose shape is more accurately represented by 2 Schechter functions, one linked to the ETG and the other to the LTG populations. For the global population, we confirm a mass-dependent evolution (“mass-assembly downsizing”), i.e., galaxy number density increases with cosmic time by a factor of two between z = 1 and z = 0 for intermediate-to-low mass (log (ℳ/ℳ⊙) ~ 10.5) galaxies but less than 15% for log (ℳ/ℳ⊙) > 11. We find that the GSMF evolution at intermediate-to-low values of ℳ (log (ℳ/ℳ⊙) < 10.6) is mostly explained by the growth in stellar mass driven by smoothly decreasing star formation activities, despite the redder colours predicted in particular at low redshift. The low residual evolution is consistent, on average, with ~0.16 merger per galaxy per Gyr (of which fewer than 0.1 are major), with a hint of a decrease with cosmic time but not a clear dependence on the mass. From the analysis of different galaxy types, we find that ETGs, regardless of the classification method, increase in number density with cosmic time more rapidly with decreasing ℳ, i.e., follow a top-down building history, with a median “building redshift” increasing with mass (z > 1 for log (ℳ/ℳ⊙) > 11), in contrast to hierarchical model predictions. For LTGs, we find that the number density of blue or spiral galaxies with log (ℳ/ℳ⊙) > 10 remains almost constant with cosmic time from z ~1. Instead, the most extreme population of star-forming galaxies (with high specific star formation), at intermediate/high-mass, rapidly decreases in number density with cosmic time. Our data can be interpreted as a combination of different effects. Firstly, we suggest a transformation, driven mainly by SFH, from blue, active, spiral galaxies of intermediate mass to blue quiescent and subsequently (1−2 Gyr after) red, passive types of low specific star formation. We find an indication that the complete morphological transformation, probably driven by dynamical processes, into red spheroidal galaxies, occurred on longer timescales or followed after 1−2 Gyr. A continuous replacement of blue galaxies is expected to be accomplished by low-mass active spirals increasing their stellar mass. We estimate the growth rate in number and mass density of the red galaxies at different redshifts and masses. The corresponding fraction of blue galaxies that, at any given time, is transforming into red galaxies per Gyr, due to the quenching of their SFR, is on average ~25% for log (ℳ/ℳ⊙) < 11. We conclude that the build-up of galaxies and in particular of ETGs follows the same downsizing trend with mass (i.e. occurs earlier for high-mass galaxies) as the formation of their stars and follows the converse of the trend predicted by current SAMs. In this scenario, we expect there to be a negligible evolution of the galaxy baryonic mass function (GBMF) for the global population at all masses and a decrease with cosmic time in the GBMF for the blue galaxy population at intermediate-high masses.

17 November 2011 in The Astrophysical Journal
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RBR. Bordoloi
R. Bordoloi
SLS. J. Lilly
S. J. Lilly
CKC. Knobel
C. Knobel
MBM. Bolzonella
M. Bolzonella
PKP. Kampczyk
P. Kampczyk
NWN. Welikala
N. Welikala