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Photometric properties of Lyα emitters at z = 4.86in the COSMOS 2 square degree field

塩谷泰広、谷口義明、長尾透 ( 愛媛大学宇宙進化研究センター ) 、井手上祐子、中島亜紀、松岡健太 ( 愛媛大学 ) 、佐々木俊二 ( 愛媛大学、東北大学 ) 、村山卓 ( 東北大学 ) 、 COSMOS チーム. Photometric properties of Lyα emitters at z = 4.86in the COSMOS 2 square degree field. ABSTRACT.

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Photometric properties of Lyα emitters at z = 4.86in the COSMOS 2 square degree field

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  1. 塩谷泰広、谷口義明、長尾透(愛媛大学宇宙進化研究センター)、井手上祐子、中島亜紀、松岡健太(愛媛大学)、佐々木俊二(愛媛大学、東北大学)、村山卓(東北大学)、塩谷泰広、谷口義明、長尾透(愛媛大学宇宙進化研究センター)、井手上祐子、中島亜紀、松岡健太(愛媛大学)、佐々木俊二(愛媛大学、東北大学)、村山卓(東北大学)、 COSMOS チーム Photometric properties of Lyα emitters at z = 4.86in the COSMOS 2 square degree field ABSTRACT We present results of a survey for Lyα emitters at z =4.86 based on optical narrowband (λC=7126 Å, Δλ=73Å) andbroadband (B, V, r’, i’, and z’) observations of the Cosmic Evolution Survey (COSMOS) field using Suprime-Cam on the Subaru Telescope. We find 79 LAE candidates at z=4.86 over a contiguous survey area of 1.83 deg2, down to the Lyα line flux of 1.47x 10-17 ergs s-1 cm-2. We obtain the Lyα luminosity function with a best-fit Schechter parameters of log L*=42.9+0.5-0.3 ergs s-1 and φ* = 1.2+8.0-1.1 x 10-4 Mpc-3 for α=-1.5 (fixed). The two-point correlation function for our LAE sample is ξ(r) = (r/4.4+5.7-2.9Mpc)-1.90±0.22. In order to investigate the field-to-field variations of the properties of Lyα emitters, we divide the survey area into nine tiles of 0.5 deg x 0.5 deg each. We find that the number density varies with a factor of ~ 2 from field to field with high statistical significance. However, we find no significant field-to-field variance when we divide the field into four tiles with 0.7 deg x 0.7 deg each. We conclude that at least 0.5 deg2 survey area is required to derive averaged properties of LAEs at z ~ 5, and our survey field is wide enough to overcome the cosmic variance. Sample • 輝線天体の選択 2.Lyα輝線天体の選択 B-dropout 79 LAEs Blue lines: Coleman, Wu, Weedman(1980), Green lines: Kinney et al. (1996)’s starburst, Red line: Bruzual & Charlot (2003)’ssynthesized SED with emission lines. サンプルの例 Results Lyα 光度関数 MUV=-21.5 の数密度 天球上の分布と相関関数 LAEs の天球上の分布灰色の領域はマスク領域。実線は面密度が平均値の 2倍の等面密度線。 0.5deg x 0.5deg で分割すると数密度の field-to-field variations はほぼ 2倍。0.7 deg x 0.7 deg ではほとんどない。 0.5deg x 0.5deg では大規模構造の影響を受けるが 0.7deg x 0.7deg では平均的な描像を得られる。 UVLF を作りMUV=-21.5での数密度を Ouchi et al. (2008) と比較したもの。 z=4.9 での数密度は z=3.1-3.7 の値より大きく z=5.7 での値に近い。 • 今回得られた光度関数を • これまでに得られている • 3 < z < 6 の光度関数と比較。 • 今回の結果も 3 < z < 6 で光度関数がほとんど進化していないという主張と矛盾しない。 Correlation length Mpc

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