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研究生: 林泓宇
Lin, Hung-Yu
論文名稱: 利用Hyper Suprime-Cam Subaru Strategic Program的光學資料研究X射線選取星系團內星系的條件光度函數
Studying the conditional luminosity function of galaxies within X-ray-selected galaxy clusters using optical data from the Hyper Suprime-Cam Subaru Strategic Program
指導教授: 邱奕儂
Chiu, I-Non
學位類別: 碩士
Master
系所名稱: 理學院 - 物理學系
Department of Physics
論文出版年: 2025
畢業學年度: 114
語文別: 英文
論文頁數: 60
中文關鍵詞: 條件光度函數星系團紅序星系星系演化
外文關鍵詞: conditional luminosity function, galaxy clusters, red-sequence galaxies, galaxy evolution
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  • 我們利用 Hyper Suprime-Cam Subaru Strategic Program(HSC-SSP)的光學測光資料,以及 eROSITA Final Equatorial-Depth Survey(eFEDS)中 X-ray 選取的星系團樣本,量測並分析星系團星系的條件光度函數(conditional luminosity functions, CLFs)。我們的最終樣本包含 346 個星系團,這些星系團是從原始的 542 個 eFEDS 星系團中篩選而得,涵蓋紅移範圍 0.1 < z < 1.2,以及質量範圍 10^13 < M500c/(M⊙/h) < 10^15。星系團質量直接採用 Chiu et al. 的結果,該研究利用弱重力透鏡與 X-ray 可觀測量進行校準。CLF 的建構僅考慮位於 r500c 內的星系,並以統計方式扣除前景與背景星系的貢獻。我們將 CLFs 依紅移分群堆疊,並在每一個紅移區間中進一步考慮兩類星系族群:完整樣本(紅色加藍色星系)以及透過事先校準的紅序模型(Chiu in prep.)進行紅–藍分離後所選取的紅序星系樣本。CLFs 以 Schechter 函數進行擬合,其中三個自由參數 (ϕ∗, α, m∗) 重新參數化為 (ϕ′, α, ∆m)。在此, ϕ′ ≡ ϕ∗M500c/Mpiv 為基準質量 Mpiv = 10^14M⊙/h 正規化後的歸一化參數,而 ∆m ≡ m∗ − m∗model 則表示特徵星等相對於紅序模型預測值的偏移量。我們使用馬可夫鏈蒙地卡羅(MCMC)方法來探索參數空間。我們的主要結果如下:(1)紅序星系族群每單位質量得歸一化參數ϕ′ 隨紅移增加呈現微弱(1.5σ)的下降趨勢;(2)完整星系族群的 m∗ 值傾向於比紅序族群更為負值;以及(3)在目前的堆疊策略下,紅序模型能夠良好地描述觀測資料。

    We measure and analyze the conditional luminosity functions (CLFs) of cluster galaxies using photometric data from the Hyper Suprime-Cam Subaru Strategic Program (HSC-SSP) and a sample of X-ray–selected galaxy clusters from the eROSITA Final Equatorial-Depth Survey (eFEDS). Our final sample consists of 346 clusters selected from an initial catalog of 542 eFEDS systems, spanning the redshift range 0.1 < z < 1.2 and halo masses 10^13 < M500c/(M⊙/h) < 10^15. The cluster masses are adopted directly from Chiu et al. , where they are calibrated using weak-lensing and X-ray observables. The CLFs are constructed using galaxies within r500c, with the fore- and background galaxy populations statistically subtracted. We stack the CLFs in redshift bins and, within each bin, consider two galaxy populations: the full (red + blue) sample and a red-sequence–selected sample obtained through red–blue separation using a pre-calibrated red-sequence model (Chiu in prep.). The CLFs are modeled with a Schechter function, in which the three free parameters (ϕ∗, α, m∗) are reparameterized as (ϕ′, α, ∆m). Here, ϕ′ ≡ ϕ∗M500c/Mpiv represents the normalization per pivot halo mass Mpiv = 10^14M⊙/h, and ∆m ≡ m∗ − m∗ model denotes the deviation of the characteristic magnitude from the value predicted by the red-sequence model. We explore the parameter space using a Markov chain Monte Carlo method. As a result, we find that (1) The normalization per pivotal mass ϕ′ of the red population has a weak (1.5σ) declining trend toward higher redshift; (2) the m∗ values of the full populations tend to be more negative than those of the red populations; and (3) the RS model provides a good description of the data under our current stacking strategy.

    Abstract in Chinese i Abstract in English ii Acknowledgements iii Contents iv List of Tables vi List of Figures vii Chapter 1 Introduction 1 Section 1.1 The structure formation in a cosmological framework 1 Section 1.2 Galaxy clusters 2 Section 1.3 The galaxy evolution in galaxy clusters 6 Section 1.4 Stellar population synthesis 10 Chapter 2 Data 12 Section 2.1 The cluster sample from the eROSITA Final Equatorial-Depth Survey 12 Section 2.2 The Hyper Suprime-Cam Subaru Strategy Program 15 Section 2.3 The red sequence model 19 Chapter 3 Method 22 Section 3.1 The selection of galaxy samples 22 Section 3.1.1 The magnitude selection 22 Section 3.1.2 The red-blue separation based on a color selection 22 Section 3.2 The statistical background subtraction 24 Section 3.3 Stacking 25 Section 3.4 Model of the conditional luminosity function 28 Section 3.5 Likelihood and prior 28 Chapter 4 Results and Discussions 31 Section 4.1 The conditional luminosity function 31 Section 4.2 The validation of the red-sequence model 37 Section 4.3 Comparisons with previous studies 37 Section 4.3.1 The normalization factor 37 Section 4.3.2 The faint-end slope 38 Section 4.3.3 The characteristic magnitude 39 Chapter 5 Conclusions 41 References 43

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