P. Melchior
Princeton University
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Featured researches published by P. Melchior.
Nature | 2012
Wei Zheng; Marc Postman; Adi Zitrin; John Moustakas; Xinwen Shu; S. Jouvel; Ole Host; A. Molino; L. Bradley; Dan Coe; Leonidas A. Moustakas; Mauricio Carrasco; Holland C. Ford; N. Benítez; Tod R. Lauer; S. Seitz; R. J. Bouwens; Anton M. Koekemoer; Elinor Medezinski; Matthias Bartelmann; Tom Broadhurst; Megan Donahue; C. Grillo; Leopoldo Infante; Saurabh W. Jha; Daniel D. Kelson; Ofer Lahav; Doron Lemze; P. Melchior; Massimo Meneghetti
Re-ionization of the intergalactic medium occurred in the early Universe at redshift z ≈ 6–11, following the formation of the first generation of stars. Those young galaxies (where the bulk of stars formed) at a cosmic age of less than about 500 million years (z ≲ 10) remain largely unexplored because they are at or beyond the sensitivity limits of existing large telescopes. Understanding the properties of these galaxies is critical to identifying the source of the radiation that re-ionized the intergalactic medium. Gravitational lensing by galaxy clusters allows the detection of high-redshift galaxies fainter than what otherwise could be found in the deepest images of the sky. Here we report multiband observations of the cluster MACS J1149+2223 that have revealed (with high probability) a gravitationally magnified galaxy from the early Universe, at a redshift of z = 9.6 ± 0.2 (that is, a cosmic age of 490 ± 15 million years, or 3.6 per cent of the age of the Universe). We estimate that it formed less than 200 million years after the Big Bang (at the 95 per cent confidence level), implying a formation redshift of ≲14. Given the small sky area that our observations cover, faint galaxies seem to be abundant at such a young cosmic age, suggesting that they may be the dominant source for the early re-ionization of the intergalactic medium.Johns Hopkins University, 3701 San Martin Drive, Baltimore , MD 21218, U.S.A. Space Telescope Science Institute Universität Heidelberg University of California, San Diego University of Science and Technology of China University College London Institute de Ciencies de l’Espai Instituto de Astrofı́sica de Andalucı́a Jet Propulsion Laboratory, California Institute of Techno logy Pontificia Universidad Católica de Chile National Optical Astronomical Observatory Universitas Sternwarte, München Leiden Observatory University of Basque Country
The Astrophysical Journal | 2014
R. J. Bouwens; L. Bradley; Adi Zitrin; D. Coe; Marijn Franx; W. Zheng; R. Smit; Ole Host; Marc Postman; Leonidas A. Moustakas; Ivo Labbé; Mauricio Carrasco; A. Molino; Megan Donahue; D. Kelson; Massimo Meneghetti; N. Benítez; Doron Lemze; Keiichi Umetsu; Tom Broadhurst; John Moustakas; P. Rosati; S. Jouvel; Matthias Bartelmann; Holland C. Ford; Genevieve J. Graves; C. Grillo; L. Infante; Y. Jimenez-Teja; Ofer Lahav
We utilise a two-color Lyman-Break selection criterion to search for z � 9-10 galaxies over the first 19 clusters in the CLASH program. Key to this search are deep observations over our clusters in five near-IR passbands to 1.6µm, allowing us good constraints on the position of the Lyman break to z � 10. A systematic search yields three z � 9-10 candidates in total above a 6� detection limit. While we have already reported the most robust of these candidates, MACS1149-JD, in a previous publication, two additional z � 9 candidates are also revealed in our expanded search. The new candidates have H160-band AB magnitudes of �26.2-26.9 and are located behind MACSJ1115.9+0129 and MACSJ1720.3+3536. The observed H160 Spitzer/IRAC colors for the sources are sufficiently blue to strongly favor redshifts of z � 9 for these sources. A careful assessment of various sources of contamination suggests .1 contaminants for our z � 9-10 selection. To determine the implications of these search results for the LF and SFR density at z � 9, we introduce a new differential approach to deriving these quantities in lensing fields. Our procedure is to derive the evolution by comparing the number of z � 9-10 galaxy candidates found in CLASH with the number of galaxies in a slightly lower redshift sample (after correcting for the differences in selection volumes), here taken to be z � 8. This procedure takes advantage of the fact that the relative selection volumes available for the z � 8 and z � 9-10 selections behind lensing clusters are not greatly dependent on the details of the gravitational lensing models. We find that the normalization of the UV LF at z � 9 is just 0.22 +0.30 −0.15 × that at z � 8, �2 +31× lower than what we would infer extrapolating z � 4-8 LF results. These results therefore suggest a more rapid evolution in the UV LF at z > 8 than seen at lower redshifts (although the current evidence here is weak). Compared to similar evolutionary findings from the HUDF, our result is much more insensitive to large-scale structure uncertainties, given our many independent sightlines on the high-redshift universe. Subject headings: galaxies: evolution — galaxies: high-redshift
The Astrophysical Journal | 2014
Keiichi Umetsu; Elinor Medezinski; M. Nonino; Julian Merten; Marc Postman; M. Meneghetti; Megan Donahue; Nicole G. Czakon; A. Molino; S. Seitz; D. Gruen; Doron Lemze; I. Balestra; N. Benítez; A. Biviano; Tom Broadhurst; Holland C. Ford; C. Grillo; Anton M. Koekemoer; P. Melchior; A. Mercurio; John Moustakas; P. Rosati; Adi Zitrin
We present a joint shear-and-magnification weak-lensing analysis of a sample of 16 X-ray-regular and 4 high-magnification galaxy clusters at 0.19 ≾ z ≾ 0.69 selected from the Cluster Lensing And Supernova survey with Hubble (CLASH). Our analysis uses wide-field multi-color imaging, taken primarily with Suprime-Cam on the Subaru Telescope. From a stacked-shear-only analysis of the X-ray-selected subsample, we detect the ensemble-averaged lensing signal with a total signal-to-noise ratio of ≃ 25 in the radial range of 200-3500 kpc h^(–1), providing integrated constraints on the halo profile shape and concentration-mass relation. The stacked tangential-shear signal is well described by a family of standard density profiles predicted for dark-matter-dominated halos in gravitational equilibrium, namely, the Navarro-Frenk-White (NFW), truncated variants of NFW, and Einasto models. For the NFW model, we measure a mean concentration of c_(200c)=4.01^(+0.35)_(-0.32) at an effective halo mass of M_(200c)=1.34^(+0.10)_(-0.09) x 10^(15)M_☉. We show that this is in excellent agreement with Λ cold dark matter (ΛCDM) predictions when the CLASH X-ray selection function and projection effects are taken into account. The best-fit Einasto shape parameter is ɑ_E=0.191^(+0.071)_(-0.068), which is consistent with the NFW-equivalent Einasto parameter of ~0.18. We reconstruct projected mass density profiles of all CLASH clusters from a joint likelihood analysis of shear-and-magnification data and measure cluster masses at several characteristic radii assuming an NFW density profile. We also derive an ensemble-averaged total projected mass profile of the X-ray-selected subsample by stacking their individual mass profiles. The stacked total mass profile, constrained by the shear+magnification data, is shown to be consistent with our shear-based halo-model predictions, including the effects of surrounding large-scale structure as a two-halo term, establishing further consistency in the context of the ΛCDM model.
Monthly Notices of the Royal Astronomical Society | 2012
Thomas D. Kitching; Sreekumar T. Balan; Sarah Bridle; N. Cantale; F. Courbin; T. F. Eifler; Marc Gentile; M. S. S. Gill; Stefan Harmeling; Catherine Heymans; Michael Hirsch; K. Honscheid; Tomasz Kacprzak; D. Kirkby; Daniel Margala; Richard Massey; P. Melchior; G. Nurbaeva; K. Patton; J. Rhodes; Barnaby Rowe; Andy Taylor; M. Tewes; Massimo Viola; Dugan Witherick; Lisa Voigt; J. Young; Joe Zuntz
We present the results from the first public blind point-spread function (PSF) reconstruction challenge, the GRavitational lEnsing Accuracy Testing 2010 (GREAT10) Star Challenge. Reconstruction of a spatially varying PSF, sparsely sampled by stars, at non-star positions is a critical part in the image analysis for weak lensing where inaccuracies in the modeled ellipticity e and size R^2 can impact the ability to measure the shapes of galaxies. This is of importance because weak lensing is a particularly sensitive probe of dark energy and can be used to map the mass distribution of large scale structure. Participants in the challenge were presented with 27,500 stars over 1300 images subdivided into 26 sets, where in each set a category change was made in the type or spatial variation of the PSF. Thirty submissions were made by nine teams. The best methods reconstructed the PSF with an accuracy of σ(e) ≈ 2.5 × 10^(–4) and σ(R^2)/R^2 ≈ 7.4 × 10^(–4). For a fixed pixel scale, narrower PSFs were found to be more difficult to model than larger PSFs, and the PSF reconstruction was severely degraded with the inclusion of an atmospheric turbulence model (although this result is likely to be a strong function of the amplitude of the turbulence power spectrum).
The Astrophysical Journal | 2014
R. Smit; R. J. Bouwens; Ivo Labbé; W. Zheng; L. Bradley; Megan Donahue; Doron Lemze; John Moustakas; Keiichi Umetsu; Adi Zitrin; D. Coe; Marc Postman; V. Gonzalez; Matthias Bartelmann; N. Benítez; Tom Broadhurst; Holland C. Ford; C. Grillo; L. Infante; Y. Jimenez-Teja; S. Jouvel; D. Kelson; Ofer Lahav; D. Maoz; Elinor Medezinski; P. Melchior; Massimo Meneghetti; Julian Merten; A. Molino; Leonidas A. Moustakas
Growing observational evidence indicates that nebular line emission has a significant impact on the rest-frame optical fluxes of z ~ 5-7 galaxies. This line emission makes z ~ 5-7 galaxies appear more massive, with lower specific star-formation rates (sSFRs). However, corrections for this line emission have been difficult to perform reliably because of huge uncertainties on the strength of such emission at z ≳ 5.5. In this paper, we present the most direct observational evidence thus far for ubiquitous high-equivalent-width (EW) [O III] + Hβ line emission in Lyman-break galaxies at z ~ 7, and we present a strategy for an improved measurement of the sSFR at z ~ 7. We accomplish this through the selection of bright galaxies in the narrow redshift window z ~ 6.6-7.0 where the Spitzer/Infrared Array Camera (IRAC) 4.5 μm flux provides a clean measurement of the stellar continuum light, in contrast with the 3.6 μm flux, which is contaminated by the prominent [O III] + Hβ lines. To ensure a high signal-to-noise ratio for our IRAC flux measurements, we consider only the brightest (H_(160) < 26 mag) magnified galaxies we have identified behind galaxy clusters. It is remarkable that the mean rest-frame optical color for our bright seven-source sample is very blue, [3.6]-[4.5] = –0.9 ± 0.3. Such blue colors cannot be explained by the stellar continuum light and require that the rest-frame EW of [O III] + Hβ is greater than 637 A for the average source. The four bluest sources from our seven-source sample require an even more extreme EW of 1582 A. We can also set a robust lower limit of ≳ 4 Gyr^(–1) on the sSFR of our sample based on the mean spectral energy distribution.
The Astrophysical Journal | 2015
Julian Merten; M. Meneghetti; Marc Postman; Keiichi Umetsu; Adi Zitrin; Elinor Medezinski; M. Nonino; Anton M. Koekemoer; P. Melchior; D. Gruen; Leonidas A. Moustakas; Matthias Bartelmann; Ole Host; Megan Donahue; D. Coe; A. Molino; S. Jouvel; A. Monna; S. Seitz; Nicole G. Czakon; Doron Lemze; Jack Sayers; I. Balestra; Piero Rosati; N. Benítez; A. Biviano; R. J. Bouwens; L. Bradley; Tom Broadhurst; Mauricio Carrasco
We present a new determination of the concentration–mass (c–M) relation for galaxy clusters based on our comprehensive lensing analysis of 19 X-ray selected galaxy clusters from the Cluster Lensing and Supernova Survey with Hubble (CLASH). Our sample spans a redshift range between 0.19 and 0.89. We combine weak-lensing constraints from the Hubble Space Telescope (HST) and from ground-based wide-field data with strong lensing constraints from HST. The results are reconstructions of the surface-mass density for all CLASH clusters on multi-scale grids. Our derivation of Navarro–Frenk–White parameters yields virial masses between 0.53 × 10^(15) M_⊙ h and 1.76 × 10^(15) M_⊙ h and the halo concentrations are distributed around c_(200c) ∼ 3.7 with a 1σ significant negative slope with cluster mass. We find an excellent 4% agreement in the median ratio of our measured concentrations for each cluster and the respective expectation from numerical simulations after accounting for the CLASH selection function based on X-ray morphology. The simulations are analyzed in two dimensions to account for possible biases in the lensing reconstructions due to projection effects. The theoretical c–M relation from our X-ray selected set of simulated clusters and the c–M relation derived directly from the CLASH data agree at the 90% confidence level.
The Astrophysical Journal | 2015
Adi Zitrin; Agnese Fabris; Julian Merten; P. Melchior; M. Meneghetti; Anton M. Koekemoer; Dan Coe; Matteo Maturi; Matthias Bartelmann; Marc Postman; Keiichi Umetsu; Gregor Seidel; Irene Sendra; Tom Broadhurst; I. Balestra; A. Biviano; C. Grillo; A. Mercurio; M. Nonino; P. Rosati; L. Bradley; Mauricio Carrasco; Megan Donahue; Holland C. Ford; Brenda Frye; John Moustakas
We present results from a comprehensive lensing analysis in HST data, of the complete CLASH cluster sample. We identify new multiple-images previously undiscovered allowing improved or first constraints on the cluster inner mass distributions and profiles. We combine these strong-lensing constraints with weak-lensing shape measurements within the HST FOV to jointly constrain the mass distributions. The analysis is performed in two different common parameterizations (one adopts light-traces-mass for both galaxies and dark matter while the other adopts an analytical, elliptical NFW form for the dark matter), to provide a better assessment of the underlying systematics - which is most important for deep, cluster-lensing surveys, especially when studying magnified high-redshift objects. We find that the typical (median), relative systematic differences throughout the central FOV are
Monthly Notices of the Royal Astronomical Society | 2012
P. Melchior; Massimo Viola
\sim40\%
The Astrophysical Journal | 2012
Dan Coe; Keiichi Umetsu; Adi Zitrin; Megan Donahue; Elinor Medezinski; Marc Postman; Mauricio Carrasco; T. Anguita; Margaret J. Geller; Kenneth Rines; Michael J. Kurtz; L. Bradley; Anton M. Koekemoer; Wei Zheng; M. Nonino; A. Molino; Andisheh Mahdavi; Doron Lemze; Leopoldo Infante; Sara Ogaz; P. Melchior; Ole Host; Holland C. Ford; C. Grillo; P. Rosati; Y. Jimenez-Teja; John Moustakas; Tom Broadhurst; Begoña Ascaso; Ofer Lahav
in the (dimensionless) mass density,
Monthly Notices of the Royal Astronomical Society | 2016
M. Jarvis; E. Sheldon; J. Zuntz; Tomasz Kacprzak; Sarah Bridle; Adam Amara; Robert Armstrong; M. R. Becker; G. M. Bernstein; C. Bonnett; C. L. Chang; Ritanjan Das; J. P. Dietrich; A. Drlica-Wagner; T. F. Eifler; C. Gangkofner; D. Gruen; Michael Hirsch; Eric Huff; Bhuvnesh Jain; S. Kent; D. Kirk; N. MacCrann; P. Melchior; A. A. Plazas; Alexandre Refregier; Barnaby Rowe; E. S. Rykoff; S. Samuroff; C. Sanchez
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