gerard kriss stsci

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the IGM: Implications for Seeing HI Re- ionization Gerard Kriss STScI

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FUSE and HST Observations of Helium II Absorption in the IGM: Implications for Seeing HI Re-ionization. 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. - PowerPoint PPT Presentation

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Page 1: Gerard Kriss STScI

FUSE and HST Observations of Helium II Absorption in the IGM: Implications for Seeing HI Re-

ionization Gerard Kriss

STScI

Page 2: Gerard Kriss STScI

What We Can Learn from Observationsof 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.

• A red damping wing on the G-P trough?

• Proximity zone on the blue side of the trough edge?

• Red-shifted absorption features indicative of infalling clouds?

Page 3: Gerard Kriss STScI

Quasars with He II Absorption

Quasar Z V Observed with:

Q 0302-003 3.29 17.8 FOC, GHRS, STIS

HS 1700+64 2.74 16.1 HUT, FOS, GHRS, STIS, FUSE

HE 234743 2.89 16.3 FOS, GHRS, STIS, FUSE

PKS 193569 3.18 17.3 GHRS, FOS

SDSS 234600 3.49 17.5 STIS, ACS

SDSS 1711+60 3.83 19.4 STIS

SDSS 1614+48 3.81 19.6 STIS

Q 1157+31 2.97 17 STIS

Difficult to seeat z~3, only 15% of sightlines are free of LLSs.

There are only 8 known quasars with clear lines of sight:

Page 4: Gerard Kriss STScI

Indirect Indicators of He II Reionization

Observations of the end stages of He II reionization: HE2347-4342: Reimers et al. (1997), Smette et al. (2002), Zheng et al. (2004a).

Si IV/C IV decreases at z~3: Songaila (1998; 2005).

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).

Page 5: Gerard Kriss STScI

He II Optical Depth vs. Redshift

Davidsen et al. 1996Smette et al. 2002Zheng et al. 2004aFechner et al. 2006

Page 6: Gerard Kriss STScI

The Transition to Complete Reionization

Redshift

Ly

Razoumov et al. 2002

Page 7: Gerard Kriss STScI

Indirect Indicators of He II Reionization

Observations of the end stages of He II reionization: HE2347-4342: Reimers et al. (1997), Smette et al. (2002), Zheng et al. (2004a).

Si IV/C IV decreases at z~3: Songaila (1998; 2005).

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).

Page 8: Gerard Kriss STScI

Ionization Evolution of the IGM

Songaila 2005(see also 1998)

Page 9: Gerard Kriss STScI

Indirect Indicators of He II Reionization

Observations of the end stages of He II reionization: HE2347-4342: Reimers et al. (1997), Smette et al. (2002), Zheng et al. (2004a).

Si IV/C IV decreases at z~3: Songaila (1998; 2005).

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).

Page 10: Gerard Kriss STScI

Thermal History of the IGM

Theuns et al. 2002

Page 11: Gerard Kriss STScI

Indirect Indicators of He II Reionization

Observations of the end stages of He II reionization: HE2347-4342: Reimers et al. (1997), Smette et al. (2002), Zheng et al. (2004a).

Si IV/C IV decreases at z~3: Songaila (1998; 2005).

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).

Page 12: Gerard Kriss STScI

Opacity Evolution of the HI Ly Forest

Bernardi et al. 2003

Page 13: Gerard Kriss STScI

IGM Optically ThickIn He II Ly

ExtrapolatedContinuum

TransparentWindows

IGM Transparent in He II Ly

Kriss et al. 2001

FUSE Spectrum of HE2347-4342

(376 ks)

Page 14: Gerard Kriss STScI

FUSE He II Absorption Keck H I

Kriss et al. 2001

Page 15: Gerard Kriss STScI

STIS & FUSE Spectra of HS1700+6416

Fechner et al. 2006

STIS Spectrum: G140L + G230LBest-fit continuum with E(B-V)=0.025

FUSE Spectrum: 290 ks

Page 16: Gerard Kriss STScI

Starlight

Quasar Illumination

(NHeII/NHI) vs. Redshift (z)

Zheng et al. 2004a

Page 17: Gerard Kriss STScI

Constraining Fesc for Star-forming Galaxies

Scott et al. 2001

Bianchi et al. 2001Scott et al. 2001Kriss & Scott 2006

Page 18: Gerard Kriss STScI

He II Absorption in SDSS QSOs

STIS Low-resolution snapshots(G140L), 600 s

(Zheng et al. 2004b)

z = 3.49

z = 3.81

z = 3.83

Page 19: Gerard Kriss STScI

Simulated He II Lyman Trough

“Cosmic voids” produced by local ionizing sources

Gunn-Peterson trough

Proximity profile

Red damping wing

He II Ly forest

Page 20: Gerard Kriss STScI

FUSE observations of HE2347–4342 and HS1700+6416 resolve the He II Ly forest.

He II / H I opacity ratios indicate that AGN contribute more than 50% of the ionizing UV flux at z=2.5.

This implies that the escape fraction for radiation from star-forming galaxies must be less than 5%.

STIS snapshots have identified 3 quasars at redshifts likely to be beyond He II reionization.

Future observations with COS of these quasars may give spectral clues to the qualitative appearance of H I reionization.

Conclusions