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首页> 外文期刊>The Astrophysical journal >HIGH-REDSHIFT QSOs IN THE SWIRE SURVEY AND THE z~3 QSO LUMINOSITY FUNCTION
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HIGH-REDSHIFT QSOs IN THE SWIRE SURVEY AND THE z~3 QSO LUMINOSITY FUNCTION

机译:线调查中的高漂移QSO和z〜3 QSO发光度函数

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We use a simple optical /infrared (IR) photometric selection of high-redshift QSOs that identifies a Lyman break in the optical photometry and requires a red IR color to distinguish QSOs from common interlopers. The search yields 100 z ~ 3 (U-dropout) QSO candidates with 19 < r' < 22 over 11.7 deg~2 in the ELAIS-N1 (EN1) and ELAIS-N2 (EN2) fields of the Spitzer Wide-area Infrared Extragalactic (SWIRE) Legacy Survey. The z ~ 3 selection is reliable, with spectroscopic follow-up of 10 candidates confirming thatthey are all QSOs at 2.83 < z < 3.44. We find that our z ~ 4 (g'-dropout) sample suffers from both unreliability and incompleteness but present seven previously unidentified QSOs at 3.50 < z < 3.89. Detailed simulations show our z ~ 3 completeness to be ~ 80%-90% from 3.0 < z < 3.5, significantly better than the ~30%-80% completeness of the SDSS at these redshifts. The resulting luminosity function extends 2 mag fainter than SDSS and has a faint-end slope of β = - 1.42 ± 0.15, consistent with values measured at lower redshift. Therefore, we see no evidence for evolution of the faint-end slope of the QSO luminosity function. Including the SDSS QSO sample, we have now directly measured the space density of QSOs responsible for ~70% of the QSO UV luminosity density at z ~ 3. We derive a maximum rate of H I photoionization from QSOs at z ~ 3.2, Γ = 4.8 × 10~(-13) s~(-1) about half of the total rate inferred through studies of the Lyα forest. Therefore, star-forming galaxies and QSOs must contribute comparably to the photoionization of H I in the inter galactic medium at z ~ 3.
机译:我们使用高红移QSO的简单光学/红外(IR)光度选择来识别光学光度学中的Lyman断裂,并需要红色IR来区分QSO与常见闯入者。在Spitzer广域红外河外的ELAIS-N1(EN1)和ELAIS-N2(EN2)场中,搜索会在11.7 deg〜2上产生19 <r'<22的100 z〜3(U丢失)QSO候选对象(SWIRE)旧版调查。 z〜3的选择是可靠的,对10个候选物进行了光谱跟踪,证实它们都是2.83 <z <3.44的QSO。我们发现我们的z〜4(g'-dropout)样本同时具有不可靠性和不完整性,但在3.50 <z <3.89处存在七个先前未确定的QSO。详细的模拟显示,我们的z〜3完整性从3.0 <z <3.5达到〜80%-90%,明显好于这些红移下SDSS的〜30%-80%完整性。产生的光度函数比SDSS弱2 mag,并且其微弱的末端斜率β=-1.42±0.15,与在较低红移下测得的值一致。因此,我们看不到有关QSO发光度函数的微弱斜率演化的证据。现在,包括SDSS QSO样品在内,我们已经直接测量了在z〜3时占QSO UV光度密度的70%的QSO的空间密度。我们在z〜3.2,Γ= 4.8时从QSO得出了最大的HI光电离率。 ×10〜(-13)s〜(-1)约占Lyα森林研究总速率的一半。因此,在z〜3时,恒星形成的星系和QSOs必须相对地促进星系间介质中H I的光电离。

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