Mass and magnification maps for the Hubble Space Telescope Frontier Fields clusters: implications for high-redshift studies
By J. Richard, M. Jauzac, M. Limousin, E. Jullo, B. Clément, H. Ebeling, Jean-Paul Kneib, H. Atek, P. Natarajan, E. Egami and 2 more. 2014
138 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Instrumentation
View Paper: https://www.semanticscholar.org/paper/a9e3c3d6fd864263869a6a2a8ea17a099806ef66
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- Richard S. Ellis
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- P. Oesch
- G. Illingworth
- J. Dunlop
- M. Franx
- P. V. van Dokkum
- Brant Robertson
Citations in the corpus
- The extreme faint end of the UV luminosity function at z ∼ 6 through gravitational telescopes: a comprehensive assessment of strong lensing uncertainties (2018, background): “…cosmic telescopes, magnifying background galaxies in the strong gravitational lensing regime, and as such offer a viable route to reach beyond the current observational limit (Maizy et al. 2010; Kneib & Natarajan 2011; Sharon et al. 2012; Postman et al. 2012; Richard et al. 2014b; Coe et al. 2015).”
- HUBBLE FRONTIER FIELDS FIRST COMPLETE CLUSTER DATA: FAINT GALAXIES AT z ∼ 5–10 FOR UV LUMINOSITY FUNCTIONS AND COSMIC REIONIZATION (2014, methodology): “…Mass Models Mass models of Abell 2744 are also made by the five independent groups: M. Bradač (PI), The Clusters As TelescopeS (CATS) team (Co-PI’s J.P Kneib, P. Natarajan; see Richard et al. 2014), J. Merten & A. Zitrin (CoPI’s), K. Sharon (PI; see Johnson et al. 2014), and L. Williams (PI).”
- The z = 9-10 galaxy population in the Hubble Frontier Fields and CLASH surveys: the z = 9 luminosity function and further evidence for a smooth decline in ultraviolet luminosity density at z≥ 8 (2016, methodology): “For the HFF fields analysed here, we have employed the CATS (Richard et al. 2014) and Zitrin LTM (Zitrin et al. 2013) lensing maps.”
- HUBBLE SPACE TELESCOPE COMBINED STRONG AND WEAK LENSING ANALYSIS OF THE CLASH SAMPLE: MASS AND MAGNIFICATION MODELS AND SYSTEMATIC UNCERTAINTIES (2014, methodology): “Other mass models for this cluster were published, both in the SL and WL regimes (e.g., Jauzac et al. 2012; Limousin et al. 2012; Diego et al. 2014; Richard et al. 2014; Johnson et al. 2014; Medezinski et al. 2013).”
- The Frontier Fields: Survey Design and Initial Results (2016, methodology): “…and new ground-based spectroscopic campaigns have greatly increased the number and accuracy of the redshifts for the background lensed FF galaxies (Wang et al. 2015, Hoag et al. 2015; Johnson et al. 2014; Richard et al. 2014; Ebeling et al. 2014; Grillo et al. 2015; Balestra et al. 2015).”
- The z ∼ 6 Luminosity Function Fainter than −15 mag from the Hubble Frontier Fields: The Impact of Magnification Uncertainties (2016, methodology): “For our magnification estimates for individual sources, we take the median of the model magnifications from the CATS (Jullo & Kneib 2009; Richard et al. 2014; Jauzac et al. 2015a,b),GLAFIC (Oguri 2010; Ishigaki et al. 2015; Kawamata et al. 2016), Sharon/Johnson (John- 5 son et al. 2014), and Zitrin…”
- Dust in the Reionization Era: ALMA Observations of a z = 8.38 Gravitationally Lensed Galaxy (2017, methodology): “Moreover a web tool11 enables us to estimate the magnification for Abell2744 YD4 from parametric high resolution models, i.e. version 3.1 of the CATS model (Richard et al. 2014), version 3 of Johnson et al. (2014), version 3 of Merten et al. (2011) and version 3 of GLAFIC (Ishigaki et al. 2015).”
- LENS MODELS AND MAGNIFICATION MAPS OF THE SIX HUBBLE FRONTIER FIELDS CLUSTERS (2014, methodology): “We fix the redshifts of image systems # 4 and 6 to the spectroscopic redshifts obtained by Richard et al. (2014).”
- New redshift z ≃ 9 galaxies in the Hubble Frontier Fields: implications for early evolution of the UV luminosity density (2014, methodology): “To derive these we have utilised the magnification map at z ' 9 produced by the CATS team3 (e.g. Richard et al. 2014) and have con- 2 www.cfht.hawaii.edu/ arnouts/LEPHARE/lephare.html 3 http://archive.stsci.edu/prepds/frontier/lensmodels c© 0000 RAS, MNRAS 000, 000–000 c© 0000 RAS, MNRAS 000,…”