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AAS_207_193_06_Kriss

Course: AAS 207, Fall 2009
School: Johns Hopkins
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Helium The II Lyman Forest Gerard Kriss STScI What We Can Learn from Observations of He II Absorption Use the ratio of He II and H I column densities to ascertain the shape of the ionizing spectrum. Do stars or quasars dominate the radiation field at z=2-3? Using the spectral shape in conjunction with proximity-effect measurements of the radiation field intensity, Set limits on the escape fraction of...

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Helium The II Lyman Forest Gerard Kriss STScI What We Can Learn from Observations of He II Absorption Use the ratio of He II and H I column densities to ascertain the shape of the ionizing spectrum. Do stars or quasars dominate the radiation field at z=2-3? Using the spectral shape in conjunction with proximity-effect measurements of the radiation field intensity, Set limits on the escape fraction of radiation from star-forming galaxies. Trace the qualitative appearance of He II reionization. This may serve as a preview of what H I reionization looks like. Look for a red damping wing on the G-P trough. Look for absorption features on the damping wing indicative of infalling clouds. Observations of He II in the IGM Difficult to seeat z~3, only 15% of sightlines are free of LLSs. There are only 7 known quasars with clear lines of sight. First detection of He II: Q0302-003, Jakobsen et al. (1994). First measurement of finite He II optical depth: HS1700+6416, Davidsen, Kriss & Zheng (1996). Observations of the end stages of He II reionization: HE2347-4342, Reimers et al. (1997). Other indirect indicators of He II reionization: Si IV/C IV decreases at z~3: Songaila (1998). HI line widths increase IGM temperature increases at z~3.3: Theuns et al. (2002). HI opacity decreases at z~3.3: Bernardi et al. (2003). FUSE observations resolve the He II Ly forest: Kriss et al. (2001). FUSE Spectrum of HE2347-4342 Transparent Windows Extrapolated Continuum (376 ks) IGM Transparent in He II Ly Kriss et al. 2001 IGM Optically Thick In He II Ly FUSE He II Absorption Keck H I Kriss et al. 2001 He II Lyman Lines are Turbulently Broadened Zheng et al. 2004a (NHeII/NHI) vs. Redshift (z) Starlight Quasar Illumination Zheng al. et 2004a STIS & FUSE Spectra of HS1700+6416 STIS Spectrum: G140L + G230L Best-fit continuum with E(B-V)=0.025 FUSE Spectrum: 290 ks Fechner et al. 2006 Comparison of FUSE and Keck Spectra of HS1700+6416 Fechner et al. 2006 (NHeII/NHI) vs. Redshift in HS1700+6416 (Uncorrected for metal-line absorbers) (Corrected for metal-line absorbers) Fechner et al. 2006 Inferred Spectral Indices Compared to QSOs Distribution of QSO spectral indices: Telfer et al. 2002 Shull et al. 2004 Constraining Fesc for Star-forming Galaxies Scott et al. 2001 Bianchi et al. 2001 Scott et al. 2001 Kriss & Scott 2006 He II Absorption at z=3.5 in SDSS J2346-0016 STIS Low-resolution snapshot (G140L), 600 s Zheng et al. 2004b A 40 ks ACS/SBC Prism spectrum was just obtained this fall. Stay Tuned! Conclusions FUSE observations of both HE23474342 and HS1700+6416 resolve the He II Ly forest in each object. For absorption with both He II and H I measurements (more than 90% of the observed He II features), the ratio =N(He II)/N(H I) lies bet...

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