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The mutually complementary Euclid and Roman galaxy redshift surveys will use Halpha- and [OIII]-selected emission line galaxies as tracers of the large scale structure at $0.9 \lesssim z \lesssim 1.9$ (Halpha) and $1.5 \lesssim z \lesssim…

The future space missions Euclid and WFIRST-AFTA will use the Halpha emission line to measure the redshifts of tens of millions of galaxies. The Halpha luminosity function at z>0.7 is one of the major sources of uncertainty in forecasting…

Astrophysics of Galaxies · Physics 2016-05-04 L. Pozzetti , C. M. Hirata , J. E. Geach , A. Cimatti , C. Baugh , O. Cucciati , A. Merson , P. Norberg , D. Shi

We present near-infrared emission line counts and luminosity functions from the HST WFC3 Infrared Spectroscopic Parallels (WISP) program for 29 fields (0.037 deg^2) observed using both the G102 and G141 grisms. Altogether we identify 1048…

We follow up emission line galaxies identified through the near-infrared slitless HST/WFC3 WISP survey with VLT/FORS2 optical spectroscopy. Over 4 WISP fields, we targetted 85 of 138 line emission objects at $0.4<z<2$ identified in WFC3…

Euclid and the Roman Space Telescope (Roman) will soon use grism spectroscopy to detect millions of galaxies via H$\alpha$ and [O III] $\lambda 5007$ emission. To better constrain the expected galaxy counts from these instruments, we use a…

Astrophysics of Galaxies · Physics 2023-01-25 Gautam Nagaraj , Robin Ciardullo , William P. Bowman , Alex Lawson , Caryl Gronwall

We forecast the linear bias for H${\rm \alpha}$-emitting galaxies at high redshift. To simulate a Euclid-like and a WFIRST-like survey, we place galaxies into a large-volume dark matter halo lightcone by sampling a library of…

Cosmology and Nongalactic Astrophysics · Physics 2019-06-04 Alexander Merson , Alex Smith , Andrew Benson , Yun Wang , Carlton Baugh

The WFC3 Infrared Spectroscopic Parallel Survey (WISP) uses the Hubble Space Telescope (HST) infrared grism capabilities to obtain slitless spectra of thousands of galaxies over a wide redshift range including the peak of star formation…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-30 H. Atek , B. Siana , C. Scarlata , M. Malkan , P. McCarthy , H. Teplitz , A. Henry , J. Colbert , C. Bridge , A. J. Bunker , A. Dressler , R. Fosbury , N. P. Hathi , C. Martin , N. R. Ross , H. Shim

We perform a simulation with Galacticus, a semi-analytical galaxy formation model, to predict the number counts of H$\alpha$ and [OIII] emitting galaxies. With a state-of-the-art N-body simulation, UNIT, we first calibrate Galacticus with…

Astrophysics of Galaxies · Physics 2019-10-28 Zhongxu Zhai , Andrew Benson , Yun Wang , Gustavo Yepes , Chia-Hsun Chuang

We present the WFC3 Infrared Spectroscopic Parallel (WISP) Survey. WISP is obtaining slitless, near-infrared grism spectroscopy of ~ 90 independent, high-latitude fields by observing in the pure parallel mode with Wide Field Camera-3 on the…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-19 H. Atek , M. Malkan , P. McCarthy , H. Teplitz , C. Scarlata , B. Siana , A. Henry , J. Colbert , N. R. Ross , C. Bridge , A. J. Bunker , A. Dressler , R. A. E. Fosbury , C. martin , H. Shim

In anticipation of the Euclid Wide and Deep Surveys, we present optical emission-line predictions at intermediate redshifts from 0.4 to 2.5. Our approach combines a mock light cone from the GAEA semi-analytic model to self-consistently…

Astrophysics of Galaxies · Physics 2024-09-25 Euclid Collaboration , L. Scharré , M. Hirschmann , G. De Lucia , S. Charlot , F. Fontanot , M. Spinelli , L. Xie , A. Feltre , V. Allevato , A. Plat , M. N. Bremer , S. Fotopoulou , L. Gabarra , B. R. Granett , M. Moresco , C. Scarlata , L. Pozzetti , L. Spinoglio , M. Talia , G. Zamorani , B. Altieri , A. Amara , S. Andreon , N. Auricchio , M. Baldi , S. Bardelli , D. Bonino , E. Branchini , M. Brescia , J. Brinchmann , S. Camera , V. Capobianco , C. Carbone , J. Carretero , S. Casas , F. J. Castander , M. Castellano , S. Cavuoti , A. Cimatti , G. Congedo , C. J. Conselice , L. Conversi , Y. Copin , L. Corcione , F. Courbin , H. M. Courtois , A. Da Silva , H. Degaudenzi , J. Dinis , M. Douspis , F. Dubath , X. Dupac , S. Dusini , M. Farina , S. Farrens , S. Ferriol , M. Frailis , E. Franceschi , S. Galeotta , B. Garilli , B. Gillis , C. Giocoli , A. Grazian , F. Grupp , L. Guzzo , S. V. H. Haugan , W. Holmes , I. Hook , F. Hormuth , A. Hornstrup , K. Jahnke , E. Keihänen , S. Kermiche , A. Kiessling , T. Kitching , B. Kubik , M. Kümmel , M. Kunz , H. Kurki-Suonio , S. Ligori , P. B. Lilje , V. Lindholm , I. Lloro , D. Maino , E. Maiorano , O. Mansutti , O. Marggraf , K. Markovic , N. Martinet , F. Marulli , R. Massey , S. Maurogordato , H. J. McCracken , E. Medinaceli , S. Mei , Y. Mellier , M. Meneghetti , E. Merlin , G. Meylan , L. Moscardini , E. Munari , S. -M. Niemi , C. Padilla , S. Paltani , F. Pasian , K. Pedersen , V. Pettorino , G. Polenta , M. Poncet , L. A. Popa , F. Raison , A. Renzi , J. Rhodes , G. Riccio , E. Romelli , M. Roncarelli , E. Rossetti , R. Saglia , D. Sapone , B. Sartoris , M. Schirmer , P. Schneider , A. Secroun , G. Seidel , S. Serrano , C. Sirignano , G. Sirri , L. Stanco , C. Surace , P. Tallada-Crespí , A. N. Taylor , H. I. Teplitz , I. Tereno , R. Toledo-Moreo , F. Torradeflot , I. Tutusaus , L. Valenziano , T. Vassallo , A. Veropalumbo , Y. Wang , J. Weller , J. Zoubian , E. Zucca , A. Biviano , M. Bolzonella , E. Bozzo , C. Burigana , C. Colodro-Conde , D. Di Ferdinando , R. Farinelli , J. Graciá-Carpio , G. Mainetti , M. Martinelli , N. Mauri , C. Neissner , A. A. Nucita , Z. Sakr , V. Scottez , M. Tenti , M. Viel , M. Wiesmann , Y. Akrami , S. Anselmi , C. Baccigalupi , M. Ballardini , M. Bethermin , A. Blanchard , S. Borgani , A. S. Borlaff , S. Bruton , R. Cabanac , A. Calabro , G. Cañas-Herrera , A. Cappi , C. S. Carvalho , G. Castignani , T. Castro , K. C. Chambers , S. Contarini , T. Contini , A. R. Cooray , J. Coupon , O. Cucciati , G. Desprez , S. Di Domizio , H. Dole , A. Díaz-S ánchez , J. A. Escartin Vigo , S. Escoffier , I. Ferrero , K. Ganga , J. García-Bellido , E. Gaztanaga , K. George , F. Giacomini , G. Gozaliasl , A. Gregorio , A. Hall , H. Hildebrandt , J. J. E. Kajava , V. Kansal , C. C. Kirkpatrick , L. Legrand , A. Loureiro , J. Macias-Perez , M. Magliocchetti , C. Mancini , F. Mannucci , R. Maoli , C. J. A. P. Martins , S. Matthew , L. Maurin , R. B. Metcalf , M. Migliaccio , P. Monaco , G. Morgante , Nicholas A. Walton , M. Pöntinen , V. Popa , C. Porciani , D. Potter , I. Risso , P. -F. Rocci , M. Sahlén , A. G. Sánchez , A. Schneider , M. Schultheis , M. Sereno , P. Simon , J. Steinwagner , G. Testera , M. Tewes , R. Teyssier , S. Toft , S. Tosi , A. Troja , M. Tucci , J. Valiviita , D. Vergani , G. Verza , I. A. Zinchenko

Forthcoming measurements of the line-intensity mapping (LIM) power spectrum (PS) are expected to provide valuable constraints on astrophysical and cosmological quantities. We focus on the [CII] luminosity function (LF) at high redshift,…

Cosmology and Nongalactic Astrophysics · Physics 2025-08-27 Elena Marcuzzo , Cristiano Porciani , Emilio Romano-Díaz , Prachi Khatri

Future galaxy redshift surveys aim to measure cosmological quantities from the galaxy power spectrum. A prime example is the detection of baryonic acoustic oscillations (BAOs), providing a standard ruler to measure the dark energy equation…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-14 J. E. Geach , A. Cimatti , W. Percival , Y. Wang , L. Guzzo , G. Zamorani , P. Rosati , L. Pozzetti , A. Orsi , C. M. Baugh , C. G. Lacey , B. Garilli , P. Franzetti , J. R. Walsh , M. Kümmel

Upcoming missions such as Euclid and the Nancy Grace Roman Space Telescope (Roman) will use emission-line selected galaxies to address a variety of questions in cosmology and galaxy evolution in the $z>1$ universe. The optimal observing…

We investigate the prospects of extending observations of high redshift QSOs to z>8 by means of a very wide-area near-infrared slitless spectroscopic survey, e.g. the planned survey with the European Space Agency's Euclid telescope. For any…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-30 Nathan Roche , Paolo Franzetti , Bianca Garilli , Giovanni Zamorani , Andrea Cimatti , Emanuel Rossetti

We present results from the largest contiguous narrow-band survey in the near-infrared. We have used WIRCam/CFHT and the lowOH2 filter (1.187$\pm$0.005 $\mu$m) to survey ~10 deg$^2$ of contiguous extragalactic sky in the SA22 field. A total…

The next generation of wide-field spectroscopic redshift surveys will map the large-scale galaxy distribution in the redshift range 0.7< z<2 to measure baryonic acoustic oscillations (BAO). The primary optical signature used in this…

Instrumentation and Methods for Astrophysics · Physics 2013-10-30 Johan Comparat , Jean-Paul Kneib , Roland Bacon , Nick J. Mostek , Jeffrey A. Newman , David J. Schlegel , Christophe Yèche

We present a sample of $\sim 1000$ emission line galaxies at $z=0.4-4.7$ from the $\sim0.7$deg$^2$ High-$z$ Emission Line Survey (HiZELS) in the Bo\"otes field identified with a suite of six narrow-band filters at $\approx 0.4-2.1$ $\mu$m.…

Astrophysics of Galaxies · Physics 2017-08-09 Jorryt Matthee , David Sobral , Philip Best , Ian Smail , Fuyan Bian , Behnam Darvish , Huub Röttgering , Xiaohui Fan

We present the luminosity function of [OII]-emitting galaxies at a median redshift of z=0.9, as measured in the deep spectroscopic data in the STIS Parallel Survey (SPS). The luminosity function shows strong evolution from the local value,…

Efficient selection of emission line galaxies at z > 1 by photometric information in wide field surveys is one of the keys for future spectroscopic surveys to constrain dark energy using the baryon acoustic oscillation (BAO) signature. Here…

We present the [OII] luminosity function measured in the redshift range 0.1<z<1.65 with unprecedented depth and accuracy. Our measurements are based on medium resolution flux-calibrated spectra of emission line galaxies with the FORS2…

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