The CALYMHA survey: Lyα luminosity function and global escape fraction of Lyα photons at z = 2.23

Abstract We present the CAlibrating LYMan-α with Hα (CALYMHA) pilot survey and new results on Lyman α (Lyα) selected galaxies at z ∼ 2. We use a custom-built Lyα narrow-band filter at the Isaac Newton Telescope, designed to provide a matched volume coverage to the z = 2.23 Hα HiZELS survey. Here, we...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2017-04, Vol.466 (1), p.1242-1258
Hauptverfasser: Sobral, David, Matthee, Jorryt, Best, Philip, Stroe, Andra, Röttgering, Huub, Oteo, Iván, Smail, Ian, Morabito, Leah, Paulino-Afonso, Ana
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container_title Monthly notices of the Royal Astronomical Society
container_volume 466
creator Sobral, David
Matthee, Jorryt
Best, Philip
Stroe, Andra
Röttgering, Huub
Oteo, Iván
Smail, Ian
Morabito, Leah
Paulino-Afonso, Ana
description Abstract We present the CAlibrating LYMan-α with Hα (CALYMHA) pilot survey and new results on Lyman α (Lyα) selected galaxies at z ∼ 2. We use a custom-built Lyα narrow-band filter at the Isaac Newton Telescope, designed to provide a matched volume coverage to the z = 2.23 Hα HiZELS survey. Here, we present the first results for the COSMOS and UDS fields. Our survey currently reaches a 3σ line flux limit of ∼4 × 10−17 erg s−1 cm−2, and a Lyα luminosity limit of ∼1042.3 erg s−1. We find 188 Lyα emitters over 7.3 × 105 Mpc3, but also find significant numbers of other line-emitting sources corresponding to He ii, C iii] and C iv emission lines. These sources are important contaminants, and we carefully remove them, unlike most previous studies. We find that the Lyα luminosity function at z = 2.23 is very well described by a Schechter function up to L Ly α ≈ 1043 erg s−1 with $L^{\ast }=10^{42.59^{+0.16}_{-0.08}}$  erg s−1, $\phi ^{\ast }=10^{-3.09^{+0.14}_{-0.34}}$  Mpc−3 and α = −1.75 ± 0.25. Above L Ly α ≈ 1043 erg s−1, the Lyα luminosity function becomes power-law like, driven by X-ray AGN. We find that Lyα-selected emitters have a high escape fraction of 37 ± 7 per cent, anticorrelated with Lyα luminosity and correlated with Lyα equivalent width. Lyα emitters have ubiquitous large (≈40 kpc) Lyα haloes, ∼2 times larger than their Hα extents. By directly comparing our Lyα and Hα luminosity functions, we find that the global/overall escape fraction of Lyα photons (within a 13 kpc radius) from the full population of star-forming galaxies is 5.1 ± 0.2 per cent at the peak of the star formation history. An extra 3.3 ± 0.3 per cent of Lyα photons likely still escape, but at larger radii.
doi_str_mv 10.1093/mnras/stw3090
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We use a custom-built Lyα narrow-band filter at the Isaac Newton Telescope, designed to provide a matched volume coverage to the z = 2.23 Hα HiZELS survey. Here, we present the first results for the COSMOS and UDS fields. Our survey currently reaches a 3σ line flux limit of ∼4 × 10−17 erg s−1 cm−2, and a Lyα luminosity limit of ∼1042.3 erg s−1. We find 188 Lyα emitters over 7.3 × 105 Mpc3, but also find significant numbers of other line-emitting sources corresponding to He ii, C iii] and C iv emission lines. These sources are important contaminants, and we carefully remove them, unlike most previous studies. We find that the Lyα luminosity function at z = 2.23 is very well described by a Schechter function up to L Ly α ≈ 1043 erg s−1 with $L^{\ast }=10^{42.59^{+0.16}_{-0.08}}$  erg s−1, $\phi ^{\ast }=10^{-3.09^{+0.14}_{-0.34}}$  Mpc−3 and α = −1.75 ± 0.25. Above L Ly α ≈ 1043 erg s−1, the Lyα luminosity function becomes power-law like, driven by X-ray AGN. 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We use a custom-built Lyα narrow-band filter at the Isaac Newton Telescope, designed to provide a matched volume coverage to the z = 2.23 Hα HiZELS survey. Here, we present the first results for the COSMOS and UDS fields. Our survey currently reaches a 3σ line flux limit of ∼4 × 10−17 erg s−1 cm−2, and a Lyα luminosity limit of ∼1042.3 erg s−1. We find 188 Lyα emitters over 7.3 × 105 Mpc3, but also find significant numbers of other line-emitting sources corresponding to He ii, C iii] and C iv emission lines. These sources are important contaminants, and we carefully remove them, unlike most previous studies. We find that the Lyα luminosity function at z = 2.23 is very well described by a Schechter function up to L Ly α ≈ 1043 erg s−1 with $L^{\ast }=10^{42.59^{+0.16}_{-0.08}}$  erg s−1, $\phi ^{\ast }=10^{-3.09^{+0.14}_{-0.34}}$  Mpc−3 and α = −1.75 ± 0.25. Above L Ly α ≈ 1043 erg s−1, the Lyα luminosity function becomes power-law like, driven by X-ray AGN. We find that Lyα-selected emitters have a high escape fraction of 37 ± 7 per cent, anticorrelated with Lyα luminosity and correlated with Lyα equivalent width. Lyα emitters have ubiquitous large (≈40 kpc) Lyα haloes, ∼2 times larger than their Hα extents. By directly comparing our Lyα and Hα luminosity functions, we find that the global/overall escape fraction of Lyα photons (within a 13 kpc radius) from the full population of star-forming galaxies is 5.1 ± 0.2 per cent at the peak of the star formation history. An extra 3.3 ± 0.3 per cent of Lyα photons likely still escape, but at larger radii.</abstract><pub>Oxford University Press</pub><doi>10.1093/mnras/stw3090</doi><tpages>17</tpages></addata></record>
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title The CALYMHA survey: Lyα luminosity function and global escape fraction of Lyα photons at z = 2.23
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