Stellar populations of lyman break galaxies at Z ≃ 1-3 in the hst/wfc3 early release science observations

Astrophysical Journal 765:2 (2013)

Authors:

RE Ryan, NP Hathi, SH Cohen, SL Finkelstein, PJ McCarthy, RA Windhorst, H Yan, AM Koekemoer, MJ Rutkowski, RW O'Connell, AN Straughn, B Balick, HE Bond, D Calzetti, MJ Disney, MA Dopita, JA Frogel, DNB Hall, JA Holtzman, RA Kimble, F Paresce, A Saha, JI Silk, JT Trauger, AR Walker, BC Whitmore, ET Young

Abstract:

We analyze the spectral energy distributions (SEDs) of Lyman break galaxies (LBGs) at z ≃ 1-3 selected using the Hubble Space Telescope (HST) Wide Field Camera 3 (WFC3) UVIS channel filters. These HST/WFC3 observations cover about 50 arcmin2 in the GOODS-South field as a part of the WFC3 Early Release Science program. These LBGs at z ≃ 1-3 are selected using dropout selection criteria similar to high-redshift LBGs. The deep multi-band photometry in this field is used to identify best-fit SED models, from which we infer the following results: (1) the photometric redshift estimate of these dropout-selected LBGs is accurate to within few percent; (2) the UV spectral slope β is redder than at high redshift (z > 3), where LBGs are less dusty; (3) on average, LBGs at z ≃ 1-3 are massive, dustier, and more highly star forming, compared to LBGs at higher redshifts with similar luminosities (0.1L* ≲ L ≲ 2.5L*), though their median values are similar within 1σ uncertainties. This could imply that identical dropout selection technique, at all redshifts, finds physically similar galaxies; and (4) the stellar masses of these LBGs are directly proportional to their UV luminosities with a logarithmic slope of ∼0.46, and star formation rates are proportional to their stellar masses with a logarithmic slope of ∼0.90. These relations hold true - within luminosities probed in this study - for LBGs from z ≃ 1.5 to 5. The star-forming galaxies selected using other color-based techniques show similar correlations at z ≃ 2, but to avoid any selection biases, and for direct comparison with LBGs at z > 3, a true Lyman break selection at z ≃ 2 is essential. The future HST UV surveys, both wider and deeper, covering a large luminosity range are important to better understand LBG properties and their evolution. © 2013. The American Astronomical Society. All rights reserved.

CFHTLenS: Testing the laws of gravity with tomographic weak lensing and redshift-space distortions

Monthly Notices of the Royal Astronomical Society 429:3 (2013) 2249-2263

Authors:

F Simpson, C Heymans, D Parkinson, C Blake, M Kilbinger, J Benjamin, T Erben, H Hildebrandt, H Hoekstra, TD Kitching, Y Mellier, L Miller, L Van Waerbeke, J Coupon, L Fu, J Harnois-Déraps, MJ Hudson, K Kuijken, B Rowe, T Schrabback, E Semboloni, S Vafaei, M Velander

Abstract:

Dark energy may be the first sign of new fundamental physics in the Universe, taking either a physical form or revealing a correction to Einsteinian gravity. Weak gravitational lensing and galaxy peculiar velocities provide complementary probes of general relativity, and in combination allow us to test modified theories of gravity in a unique way.We perform such an analysis by combining measurements of cosmic shear tomography from the Canada-France- Hawaii Telescope Lensing Survey (CFHTLenS) with the growth of structure from theWiggleZ Dark Energy Survey and the Six-degree-Field Galaxy Survey, producing the strongest existing joint constraints on the metric potentials that describe general theories of gravity. For scaleindependent modifications to the metric potentials which evolve linearly with the effective dark energy density, we find present-day cosmological deviations in the Newtonian potential and curvature potential from the prediction of general relativity to be δψ/ψ = 0.05 ± 0.25 and δφ/φ=-0.05 ± 0.3, respectively (68 per cent confidence limits). © 2012 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society.

CPEB1 coordinates alternative 3′-UTR formation with translational regulation

Nature Springer Nature 495:7439 (2013) 121-125

Authors:

Felice-Alessio Bava, Carolina Eliscovich, Pedro G Ferreira, Belen Miñana, Claudia Ben-Dov, Roderic Guigó, Juan Valcárcel, Raúl Méndez

Statistical properties of thermal Sunyaev–Zel'dovich maps

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 429:2 (2013) 1564-1584

Authors:

Dipak Munshi, Shahab Joudaki, Joseph Smidt, Peter Coles, Scott T Kay

Origins of weak lensing systematics, and requirements on future instrumentation (or knowledge of instrumentation)

Monthly Notices of the Royal Astronomical Society 429:1 (2013) 661-678

Authors:

R Massey, H Hoekstra, T Kitching, J Rhodes, M Cropper, J Amiaux, D Harvey, Y Mellier, M Meneghetti, L Miller, S Paulin-Henriksson, S Pires, R Scaramella, T Schrabback

Abstract:

The first half of this paper explores the origin of systematic biases in the measurement of weak gravitational lensing. Compared to previous work, we expand the investigation of point spread function instability and fold in for the first time the effects of non-idealities in electronic imaging detectors and imperfect galaxy shape measurement algorithms. Together, these now explain the additive A(l) and multiplicative M(l) systematics typically reported in current lensing measurements. We find that overall performance is driven by a product of a telescope/camera's absolute performance, and our knowledge about its performance. The second half of this paper propagates any residual shear measurement biases through to their effect on cosmological parameter constraints. Fully exploiting the statistical power of Stage IV weak lensing surveys will require additive biasesA 1.8 × 10-12 and multiplicative biases M 4.0 × -3. These can be allocated between individual budgets in hardware, calibration data and software, using results from the first half of the paper. If instrumentation is stable and well calibrated, we find extant shear measurement software from Gravitational Lensing Accuracy Testing 2010 (GREAT10) already meet requirements on galaxies detected at signal-to-noise ratio = 40. Averaging over a population of galaxies with a realistic distribution of sizes, it also meets requirements for a 2D cosmic shear analysis from space. If used on fainter galaxies or for 3D cosmic shear tomography, existing algorithms would need calibration on simulations to avoid introducing bias at a level similar to the statistical error. Requirements on hardware and calibration data are discussed in more detail in a companion paper. Our analysis is intentionally general, but is specifically being used to drive the hardware and ground segment performance budget for the design of the European Space Agency's recently selected Euclid mission. ©2012 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society.