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Published December 10, 2013 | Submitted + Published
Journal Article Open

Predicting Future Space Near-IR Grism Surveys using the WFC3 Infrared Spectroscopic Parallels Survey

Abstract

We present near-infrared emission line counts and luminosity functions from the Hubble Space Telescope Wide Field Camera 3 Infrared Spectroscopic Parallels (WISP) program for 29 fields (0.037 deg^2) observed using both the G102 and G141 grism. Altogether we identify 1048 emission line galaxies with observed equivalent widths greater than 40 Å, 467 of which have multiple detected emission lines. We use simulations to correct for significant (>20%) incompleteness introduced in part by the non-dithered, non-rotated nature of the grism parallels. The WISP survey is sensitive to fainter flux levels ((3-5) × 10^(–17) erg s^(–1) cm^(–2)) than the future space near-infrared grism missions aimed at baryonic acoustic oscillation cosmology ((1-4) × 10^(–16) erg s^(–1) cm^(–2)), allowing us to probe the fainter emission line galaxies that the shallower future surveys may miss. Cumulative number counts of 0.7 < z < 1.5 galaxies reach 10,000 deg^(–2) above an Hα flux of 2 × 10^(–16) erg s^(–1) cm^(–2). Hα-emitting galaxies with comparable [O III] flux are roughly five times less common than galaxies with just Hα emission at those flux levels. Galaxies with low Hα/[O III] ratios are very rare at the brighter fluxes that future near-infrared grism surveys will probe; our survey finds no galaxies with Hα/[O III] < 0.95 that have Hα flux greater than 3 × 10^(–16) erg s^(–1) cm^(–2). Our Hα luminosity function contains a comparable number density of faint line emitters to that found by the Near IR Camera and Multi-Object Spectrometer near-infrared grism surveys, but significantly fewer (factors of 3-4 less) high-luminosity emitters. We also find that our high-redshift (z = 0.9-1.5) counts are in agreement with the high-redshift (z = 1.47) narrowband Hα survey of HiZELS (Sobral et al.), while our lower redshift luminosity function (z = 0.3-0.9) falls slightly below their z = 0.84 result. The evolution in both the Hα luminosity function from z = 0.3-1.5 and the [O III] luminosity function from z = 0.7-2.3 is almost entirely in the L_* parameter, which steadily increases with redshift over those ranges.

Additional Information

© 2013 American Astronomical Society. Received 2013 May 6; accepted 2013 October 19; published 2013 November 22. We would like to acknowledge the assistance of Chun Ly for his helpful advice during the production of this paper. The authors would also like to acknowledge financial support from the grants for HST programs GO-10226, GO-11696, and GO-12283.

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Published - 0004-637X_779_1_34.pdf

Submitted - 1305.1399v1.pdf

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Created:
August 19, 2023
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October 23, 2023