MEASUREMENT OF GALAXY CLUSTERING AT z ∼ 7.2 AND THE EVOLUTION OF GALAXY BIAS FROM 3.8 < z < 8 IN THE XDF, GOODS-S, AND GOODS-N

MEASUREMENT OF GALAXY CLUSTERING AT z ∼ 7.2 AND THE EVOLUTION OF GALAXY BIAS FROM 3.8 < z < 8 IN THE XDF, GOODS-S, AND GOODS-N
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XDF、GOODS-S 和 Goods-N 中 z 〜 7.2 处星系团的测量以及从 3.8 < z < 8 开始星系偏置的演化

DOI:
10.1088/0004-637x/793/1/17
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发表时间:
2014
期刊:
The Astrophysical Journal
影响因子:
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通讯作者:
P. V. Dokkum
P. V. Dokkum
中科院分区:
--
文献类型:
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作者:
R. Barone;M. Trenti;J. Wyithe;R. Bouwens;P. Oesch;P. Oesch;G. Illingworth;C. Carollo;Jian Su;M. Stiavelli;I. Labbé;P. V. Dokkum

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Lyman-break galaxy (LBG) samples observed during reionization (z ≳ 6) with the Hubble Space Telescope's Wide Field Camera 3 are reaching sizes sufficient to characterize their clustering properties. Using a combined catalog from the Hubble eXtreme Deep Field and CANDELS surveys, containing N = 743 LBG candidates at z ⩾ 6.5 at a mean redshift of , we detect a clear clustering signal in the angular correlation function (ACF) at ≳ 4σ, corresponding to a real-space correlation length cMpc. The derived galaxy bias is that of dark matter halos of at z = 7.2, and highlights that galaxies below the current detection limit (MAB ∼ −17.7) are expected in lower-mass halos (M ∼ 108–1010.5 ). We compute the ACF of LBGs at z ∼ 3.8 − z ∼ 5.9 in the same surveys. A trend of increasing bias is found from (b ∼ 3.0) to (b ∼ 8.6), broadly consistent with galaxies at fixed luminosity being hosted in dark matter halos of similar mass at 4 ≲ z ≲ 6, followed by a slight rise in halo masses at z ≳ 7 (∼2σ confidence). Separating the data at the median luminosity of the sample (MUV = −19.4) shows higher clustering at for bright galaxies (cMpc, ) compared to faint galaxies (cMpc, ) implying a constant mass-to-light ratio . A similar trend is present in the sample with larger uncertainty. Finally, our bias measurements allow us to investigate the fraction of dark matter halos hosting UV-bright galaxies (the duty cycle, ϵDC). At values near unity are preferred, which may be explained by the shortened halo assembly time at high redshift.