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Featured researches published by M. Radovich.


Nature | 2008

A test of the nature of cosmic acceleration using galaxy redshift distortions

L. Guzzo; M. Pierleoni; B. Meneux; E. Branchini; O. Le Fèvre; C. Marinoni; B. Garilli; Jeremy Blaizot; G. De Lucia; A. Pollo; H. J. McCracken; D. Bottini; V. Le Brun; D. Maccagni; J. P. Picat; R. Scaramella; M. Scodeggio; L. Tresse; G. Vettolani; A. Zanichelli; C. Adami; S. Arnouts; S. Bardelli; M. Bolzonella; A. Bongiorno; A. Cappi; S. Charlot; P. Ciliegi; T. Contini; O. Cucciati

Observations of distant supernovae indicate that the Universe is now in a phase of accelerated expansion the physical cause of which is a mystery. Formally, this requires the inclusion of a term acting as a negative pressure in the equations of cosmic expansion, accounting for about 75 per cent of the total energy density in the Universe. The simplest option for this ‘dark energy’ corresponds to a ‘cosmological constant’, perhaps related to the quantum vacuum energy. Physically viable alternatives invoke either the presence of a scalar field with an evolving equation of state, or extensions of general relativity involving higher-order curvature terms or extra dimensions. Although they produce similar expansion rates, different models predict measurable differences in the growth rate of large-scale structure with cosmic time. A fingerprint of this growth is provided by coherent galaxy motions, which introduce a radial anisotropy in the clustering pattern reconstructed by galaxy redshift surveys. Here we report a measurement of this effect at a redshift of 0.8. Using a new survey of more than 10,000 faint galaxies, we measure the anisotropy parameter β = 0.70 ± 0.26, which corresponds to a growth rate of structure at that time of f = 0.91 ± 0.36. This is consistent with the standard cosmological-constant model with low matter density and flat geometry, although the error bars are still too large to distinguish among alternative origins for the accelerated expansion. The correct origin could be determined with a further factor-of-ten increase in the sampled volume at similar redshift.


The Astrophysical Journal | 2005

The GALEX-VVDS measurement of the evolution of the far-ultraviolet luminosity density and the cosmic star formation rate

David Schiminovich; O. Ilbert; S. Arnouts; B. Milliard; L. Tresse; O. Le Fèvre; Marie Treyer; Ted K. Wyder; Tamas Budavari; E. Zucca; G. Zamorani; D. C. Martin; C. Adami; M. Arnaboldi; S. Bardelli; Tom A. Barlow; Luciana Bianchi; M. Bolzonella; D. Bottini; Yong-Ik Byun; A. Cappi; T. Contini; S. Charlot; J. Donas; Karl Forster; S. Foucaud; P. Franzetti; Peter G. Friedman; B. Garilli; I. Gavignaud

In a companion paper (Arnouts et al. 2004) we presented new measurements of the galaxy luminosity function at 1500 Angstroms out to z~1 using GALEX-VVDS observations (1039 galaxies with NUV 0.2) and at higher z using existing data sets. In this paper we use the same sample to study evolution of the FUV luminosity density. We detect evolution consistent with a (1+z)^{2.5+/-0.7} rise to z~1 and (1+z)^{0.5+/-0.4} for z>1. The luminosity density from the most UV-luminous galaxies (UVLG) is undergoing dramatic evolution (x30) between 025%) of the total FUV luminosity density at z<1. We measure dust attenuation and star formation rates of our sample galaxies and determine the star formation rate density as a function of redshift, both uncorrected and corrected for dust. We find good agreement with other measures of the SFR density in the rest ultraviolet and Halpha given the still significant uncertainties in the attenuation correction.


Astronomische Nachrichten | 2005

GaBoDS: The Garching-Bonn Deep Survey. IV. Methods for the image reduction of multi-chip cameras demonstrated on data from the ESO Wide-Field Imager

Thomas Erben; Mischa Schirmer; J. P. Dietrich; O. Cordes; L. Haberzettl; Marco Hetterscheidt; Hendrik Hildebrandt; O. Schmithuesen; Peter Schneider; Patrick Simon; E. Deul; R. N. Hook; Nick Kaiser; M. Radovich; C. Benoist; M. Nonino; L. F. Olsen; I. Prandoni; R. Wichmann; S. Zaggia; Dominik J. Bomans; R.-J. Dettmar; J. M. Miralles

We present our image processing system for the reduction of optical imaging data from multi-chip cameras. In the framework of the Garching Bonn Deep Survey (GaBoDS; Schirmer et al. 2003) consisting of about 20 square degrees of high-quality data from WFI@MPG/ESO 2.2m, our group developed an imaging pipeline for the homogeneous and efficient processing of thislarge data set. Having weak gravitational lensing as the main science driver, our algorithms are optimised to produce deep co-added mosaics from individual exposures obtained from empty field observations. However, the modular design of our pipeline allows an easy adaption to different scientific applications. Our system has already been ported to a large variety of optical instruments and its products have been used in various scientific contexts. In this paper we give a thorough description of the algorithms used and a careful evaluation of the accuracies reached. This concerns the removal of the instrumental signature, the astrometric alignment, photometric calibration and the characterisation of final co-added mosaics. In addition we give a more general overview on the image reduction process and comment on observing strategies where they have significant influence on the data quality.


Astronomy and Astrophysics | 2005

The VIMOS-VLT Deep Survey: Evolution of the galaxy luminosity function up to z=2 in first epoch data

O. Ilbert; L. Tresse; E. Zucca; S. Bardelli; S. Arnouts; G. Zamorani; L. Pozzetti; D. Bottini; B. Garilli; V. Le Brun; O. Le Fèvre; D. Maccagni; J. P. Picat; R. Scaramella; M. Scodeggio; G. Vettolani; Alessandra Zanichelli; C. Adami; M. Arnaboldi; M. Bolzonella; A. Cappi; S. Charlot; T. Contini; Sylvie Foucaud; P. Franzetti; I. Gavignaud; L. Guzzo; A. Iovino; H. J. McCracken; B. Marano

We investigate the evolution of the galaxy luminosity function from the VIMOS-VLT Deep Survey (VVDS) from the present to z=2 in five (U, B, V, R and I) rest-frame band-passes. We use the first epoch VVDS deep sample of 11,034 spectra selected at 17.5 <= I_{AB} <= 24.0, on which we apply the Algorithm for Luminosity Function (ALF), described in this paper. We observe a substantial evolution with redshift of the global luminosity functions in all bands. From z=0.05 to z=2, we measure a brightening of the characteristic magnitude M* included in the magnitude range 1.8-2.5, 1.7-2.4, 1.2-1.9, 1.1-1.8 and 1.0-1.6 in the U, B, V, R and I rest-frame bands, respectively. We confirm this differential evolution of the luminosity function with rest-frame wavelength, from the measurement of the comoving density of bright galaxies (M < M*(z=0.1)). This density increases by a factor of around 2.6, 2.2, 1.8, 1.5, 1.5 between z=0.05 and z=1 in the U, B, V, R, I bands, respectively. We also measure a possible steepening of the faint-end slope of the luminosity functions, with \\Delta\\alpha ~ -0.3 between z=0.05 and z=1, similar in all bands.


arXiv: Astrophysics | 2005

GaBoDS: The Garching-Bonn Deep Survey IV. Methods for the Image reduction of multi-chip Cameras ⋆

Thomas Erben; Mischa Schirmer; J. P. Dietrich; O. Cordes; Lutz Haberzettl; Marco Hetterscheidt; Olaf Schmithuesen; Peter Schneider; Patrick Simon; J. C. Cuillandre; E. Deul; R. N. Hook; M. Radovich; Christophe Benoist; M. Nonino; L. F. Olsen; I. Prandoni; R. Wichmann; D. J. Bomans; R.-J. Dettmar; J. M. Miralles

We present our image processing system for the reduction of optical imaging data from multi-chip cameras. In the framework of the Garching Bonn Deep Survey (GaBoDS; Schirmer et al. 2003) consisting of about 20 square degrees of high-quality data from WFI@MPG/ESO 2.2m, our group developed an imaging pipeline for the homogeneous and efficient processing of thislarge data set. Having weak gravitational lensing as the main science driver, our algorithms are optimised to produce deep co-added mosaics from individual exposures obtained from empty field observations. However, the modular design of our pipeline allows an easy adaption to different scientific applications. Our system has already been ported to a large variety of optical instruments and its products have been used in various scientific contexts. In this paper we give a thorough description of the algorithms used and a careful evaluation of the accuracies reached. This concerns the removal of the instrumental signature, the astrometric alignment, photometric calibration and the characterisation of final co-added mosaics. In addition we give a more general overview on the image reduction process and comment on observing strategies where they have significant influence on the data quality.


The Astrophysical Journal | 2005

The GALEX VIMOS-VLT Deep Survey Measurement of the Evolution of the 1500 Å Luminosity Function

S. Arnouts; David Schiminovich; O. Ilbert; L. Tresse; B. Milliard; Marie Treyer; S. Bardelli; Tamas Budavari; Ted K. Wyder; E. Zucca; O. Le Fèvre; D. C. Martin; Giampaolo Vettolani; C. Adami; M. Arnaboldi; Tom A. Barlow; Luciana Bianchi; M. Bolzonella; D. Bottini; Yong-Ik Byun; A. Cappi; S. Charlot; T. Contini; J. Donas; Karl Forster; Sylvie Foucaud; P. Franzetti; Peter G. Friedman; B. Garilli; I. Gavignaud

We present the first measurement of the galaxy luminosity function (LF) at 1500 A in the range 0.2 ≤ z ≤ 1.2 based on Galaxy Evolution Explorer VIMOS-VLT Deep Survey observations (~1000 spectroscopic redshifts for galaxies with NUV ≤ 24.5) and at higher z using existing data sets. Our main results are summarized as follows: (1) Luminosity evolution is observed with ΔM* ~ -2.0 mag between z = 0 and z = 1 and ΔM* ~ -1.0 mag between z = 1 and z = 3. This confirms that the star formation activity was significantly higher in the past. (2) The LF slopes vary in the range -1.2 ≥ α ≥ -1.65, with a marginally significant hint of increase at higher z. (3) We split the sample in three rest-frame (B - I) intervals, providing an approximate spectral type classification: Sb-Sd, Sd-Irr, and unobscured starbursts. We find that the bluest class evolves less strongly in luminosity than the two other classes. On the other hand, their number density increases sharply with z (~15% in the local universe to ~55% at z ~ 1), while that of the reddest classes decreases.


Publications of the Astronomical Society of the Pacific | 2005

The VVDS data reduction pipeline: introducing VIPGI, the VIMOS Interactive Pipeline and Graphical Interface

M. Scodeggio; P. Franzetti; B. Garilli; A. Zanichelli; S. Paltani; D. Maccagni; D. Bottini; V. Le Brun; T. Contini; R. Scaramella; C. Adami; S. Bardelli; E. Zucca; L. Tresse; O. Ilbert; S. Foucaud; A. Iovino; R. Merighi; G. Zamorani; I. Gavignaud; D. Rizzo; H. J. McCracken; O. Le Fèvre; J. P. Picat; G. Vettolani; M. Arnaboldi; S. Arnouts; M. Bolzonella; A. Cappi; S. Charlot

The VIMOS VLT Deep Survey (VVDS), designed to measure 150,000 galaxy redshifts, requires a dedicated data reduction and analysis pipeline to process in a timely fashion the large amount of spectroscopic data being produced. This requirement has lead to the development of the VIMOS Interactive Pipeline and Graphical Interface (VIPGI), a new software package designed to simplify to a very high degree the task of reducing astronomical data obtained with VIMOS, the imaging spectrograph built by the VIRMOS Consortium for the European Southern Observatory, and mounted on Unit 3 (Melipal) of the Very Large Telescope (VLT) at Paranal Observatory (Chile). VIPGI provides the astronomer with specially designed VIMOS data reduction functions, a VIMOS-centric data organizer, and dedicated data browsing and plotting tools, that can be used to verify the quality and accuracy of the various stages of the data reduction process. The quality and accuracy of the data reduction pipeline are comparable to those obtained using well known IRAF tasks, but the speed of the data reduction process is significantly increased, thanks to the large set of dedicated features. In this paper we discuss the details of the MOS data reduction pipeline implemented in VIPGI, as applied to the reduction of some 20,000 VVDS spectra, assessing quantitatively the accuracy of the various reduction steps. We also provide a more general overview of VIPGI capabilities, a tool that can be used for the reduction of any kind of VIMOS data.


Astronomy and Astrophysics | 2009

The VIMOS VLT Deep Survey - Evolution of the major merger rate since z ~ 1 from spectroscopically confirmed galaxy pairs

L. de Ravel; O. Le Fèvre; L. Tresse; D. Bottini; B. Garilli; V. Le Brun; D. Maccagni; R. Scaramella; M. Scodeggio; G. Vettolani; A. Zanichelli; C. Adami; Stephane Arnouts; S. Bardelli; M. Bolzonella; A. Cappi; S. Charlot; P. Ciliegi; T. Contini; Sylvie Foucaud; P. Franzetti; I. Gavignaud; L. Guzzo; O. Ilbert; A. Iovino; F. Lamareille; H. J. McCracken; B. Marano; Christian Marinoni; A. Mazure

Context: The rate at which galaxies grow via successive mergers is a key element in understanding the main phases of galaxy evolution. Aims: We measure the evolution of the fraction of galaxies in pairs and the merging rate since redshift z 1 assuming a (H0 = 70 km s-1 Mpc-1, ΩM = 0.3 and ΩΛ = 0.7) cosmology. Methods: From the VIMOS VLT Deep Survey we use a sample of 6464 galaxies with I_AB ≤ 24 to identify 314 pairs of galaxies, each member with a secure spectroscopic redshift, which are close in both projected separation and in velocity. Results: We estimate that at z 0.9, 10.9 ± 3.2% of galaxies with MB(z) ≤ -18-Qz (Q = 1.11) are in pairs with separations Δ rp ≤ 20 h-1 kpc, Δ v≤ 500 km s-1, and with Δ MB ≤ 1.5, significantly larger than 3.8 ± 1.7% at z 0.5; thus, the pair fraction evolves as (1 + z)m with m = 4.73 ± 2.01. For bright galaxies with MB(z = 0) ≤ -18.77, the pair fraction is higher and its evolution with redshift is flatter with m = 1.50 ± 0.76, a property also observed for galaxies with increasing stellar masses. Early-type pairs (dry mergers) increase their relative fraction from 3% at z 0.9 to 12% at z 0.5. The star formation rate traced by the rest-frame [OII] EW increases by 26 ± 4% for pairs with the smallest separation rp ≤ 20 h-1 kpc. Following published prescriptions to derive merger timescales, we find that the merger rate of MB(z) ≤ -18-Qz galaxies evolves as N_mg = (4.96 ± 2.07)×10-4×(1 + z)2.20 ± 0.77 mergers Mpc-3 Gyr-1. Conclusions: The merger rate of galaxies with MB(z) ≤ -18-Qz has significantly evolved since z 1 and is strongly dependent on the luminosity or stellar mass of galaxies. The major merger rate increases more rapidly with redshift for galaxies with fainter luminosities or stellar mass, while the evolution of the merger rate for bright or massive galaxies is slower, indicating that the slow evolution reported for the brightest galaxies is not universal. The merger rate is also strongly dependent on the spectral type of galaxies involved. Late-type mergers were more frequent in the past, while early-type mergers are more frequent today, contributing to the rise in the local density of early-type galaxies. About 20% of the stellar mass in present day galaxies with log(M/M{ȯ}) ≥ 9.5 has been accreted through major merging events since z = 1. This indicates that major mergers have contributed significantly to the growth in stellar mass density of bright galaxies over the last half of the life of the Universe. based on observations obtained with the European Southern Observatory Telescopes at the Paranal Observatory, under programs 072.A-0586 and 073.A-0647.


Monthly Notices of the Royal Astronomical Society | 2015

Gravitational lensing analysis of the Kilo-Degree Survey

Konrad Kuijken; Catherine Heymans; Hendrik Hildebrandt; Reiko Nakajima; Thomas Erben; Jelte T. A. de Jong; Massimo Viola; Ami Choi; Henk Hoekstra; Lance Miller; Edo van Uitert; Alexandra Amon; Chris Blake; Margot M. Brouwer; Axel Buddendiek; Ian Fenech Conti; Martin Eriksen; A. Grado; Joachim Harnois-Déraps; Ewout Helmich; Ricardo Herbonnet; Nancy Irisarri; Thomas D. Kitching; Dominik Klaes; Francesco La Barbera; N. R. Napolitano; M. Radovich; Peter Schneider; Cristóbal Sifón; Gert Sikkema

The Kilo-Degree Survey (KiDS) is a multi-band imaging survey designed for cosmological studies from weak lensing and photometric redshifts. It uses the European Southern Observatory VLT Survey Telescope with its wide-field camera OmegaCAM. KiDS images are taken in four filters similar to the Sloan Digital Sky Survey ugri bands. The best seeing time is reserved for deep r-band observations. The median 5σ limiting AB magnitude is 24.9 and the median seeing is below 0.7 arcsec. Initial KiDS observations have concentrated on the Galaxy and Mass Assembly (GAMA) regions near the celestial equator, where extensive, highly complete redshift catalogues are available. A total of 109 survey tiles, 1 square degree each, form the basis of the first set of lensing analyses of halo properties of GAMA galaxies. Nine galaxies per square arcminute enter the lensing analysis, for an effective inverse shear variance of 69 arcmin-2. Accounting for the shape measurement weight, the median redshift of the sources is 0.53. KiDS data processing follows two parallel tracks, one optimized for weak lensing measurement and one for accurate matched-aperture photometry (for photometric redshifts). This technical paper describes the lensing and photometric redshift measurements (including a detailed description of the Gaussian aperture and photometry pipeline), summarizes the data quality and presents extensive tests for systematic errors that might affect the lensing analyses. We also provide first demonstrations of the suitability of the data for cosmological measurements, and describe our blinding procedure for preventing confirmation bias in the scientific analyses. The KiDS catalogues presented in this paper are released to the community through http://kids.strw.leidenuniv.nl.


Astronomy and Astrophysics | 2006

The VIMOS-VLT deep survey - evolution of the luminosity functions by galaxy type up to z = 1.5 from first epoch data

E. Zucca; O. Ilbert; S. Bardelli; L. Tresse; G. Zamorani; S. Arnouts; L. Pozzetti; M. Bolzonella; H. J. McCracken; D. Bottini; B. Garilli; V. Le Brun; O. Le Fèvre; D. Maccagni; J. P. Picat; R. Scaramella; M. Scodeggio; G. Vettolani; A. Zanichelli; C. Adami; M. Arnaboldi; A. Cappi; S. Charlot; P. Ciliegi; T. Contini; Sylvie Foucaud; P. Franzetti; I. Gavignaud; L. Guzzo; A. Iovino

From the first epoch observations of the VVDS up to z=1.5 we have derived luminosity functions (LF) of different spectral type galaxies. The VVDS data, covering ~70% of the life of the Universe, allow for the first time to study from the same sample and with good statistical accuracy the evolution of the LFs by galaxy type in several rest frame bands from a purely magnitude selected sample. The magnitude limit of the VVDS allows the determination of the faint end slope of the LF with unprecedented accuracy. Galaxies have been classified in four spectral classes, using their colours and redshift, and LFs have been derived in the U, B, V, R and I rest frame bands from z=0.05 to z=1.5. We find a significant steepening of the LF going from early to late types. The M* parameter is significantly fainter for late type galaxies and this difference increases in the redder bands. Within each of the galaxy spectral types we find a brightening of M* with increasing redshift, ranging from =< 0.5 mag for early type galaxies to ~1 mag for the latest type galaxies, while the slope of the LF of each spectral type is consistent with being constant with redshift. The LF of early type galaxies is consistent with passive evolution up to z~1.1, while the number of bright early type galaxies has decreased by ~40% from z~0.3 to z~1.1. We also find a strong evolution in the normalization of the LF of latest type galaxies, with an increase of more than a factor 2 from z~0.3 to z~1.3: the density of bright late type galaxies in the same redshift range increases of a factor ~6.6. These results indicate a strong type-dependent evolution and identifies the latest spectral types as responsible for most of the evolution of the UV-optical luminosity function out to z=1.5.

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O. Le Fèvre

Aix-Marseille University

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H. J. McCracken

Institut d'Astrophysique de Paris

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