A Deep Narrowband Imaging Search for C IV and He II Emission from Lyα Blobs

A Deep Narrowband Imaging Search for C IV and He II Emission from Lyα Blobs
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Lyα 斑点的 C IV 和 He II 发射的深窄带成像搜索

DOI:
10.1088/0004-637x/804/1/26
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发表时间:
2015
期刊:
The Astrophysical Journal
影响因子:
--
通讯作者:
Tomoki
Tomoki
中科院分区:
--
文献类型:
--
作者:
Arrigoni Battaia;Fabrizio; Yang;Yujin; Hennawi;Joseph F.; Prochaska;J. Xavier; Matsuda;Yuichi; Yamada;Toru; Hayashino;Tomoki

文献摘要

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We conduct a deep narrowband imaging survey of 13 Lyα blobs (LABs) located in the SSA22 proto-cluster at z∼ 3.1 in the C iv and He ii emission lines in an effort to constrain the physical process powering the Lyα emission in LABs. Our observations probe down to unprecedented surface brightness (SB) limits of (2.1–3.4)× 10− 18 erg s− 1 cm− 2 arcsec− 2 per 1 arcsec 2 aperture (5σ) for the He ii λ1640 and C iv λ1549 lines, respectively. We do not detect extended He ii and C iv emission in any of the LABs, placing strong upper limits on the He ii/Lyα and C iv/Lyα line ratios, of 0.11 and 0.16, for the brightest two LABs in the field. We conduct detailed photoionization modeling of the expected line ratios and find that, although our data constitute the deepest ever observations of these lines, they are still not deep enough to rule out a scenario where the Lyα emission is powered by the ionizing radiation from an obscured active galactic nucleus. Our models can accommodate He ii/Lyα and C iv/Lyα ratios as low as≃ 0.05 and≃ 0.07, respectively, implying that one needs to reach SB as low as (1–1.5)× 10− 18 erg s− 1 cm− 2 arcsec− 2(at 5σ) in order to rule out a photoionization scenario. These depths will be achievable with the new generation of image-slicing integral field units such as the Multi Unit Spectroscopic Explorer (MUSE) on VLT and the Keck Cosmic Web Imager (KCWI). We also model the expected He ii/Lyα and C iv/Lyα in a different scenario, where Lyα emission is powered by shocks generated in a large-scale superwind, but find that our observational constraints can only be met for shock velocities v s≳ 250 km s− 1, which appear to be in conflict with recent observations of quiescent kinematics in LABs.