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Tom Theuns Institute for Computational Cosmology, Durham, U Department of Physics, Antwerp, Belgium Munich 2005 Reionization Reionization And the thermal history And the thermal history of the IGM of the IGM Tom Theuns Institute for Computational Cosmology, Durham, U Department of Physics, Antwerp, Belgium

Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

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Page 1: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom TheunsInstitute for Computational Cosmology, Durham, UKDepartment of Physics, Antwerp, Belgium

Munich 2005

ReionizationReionizationAnd the thermal history of the IGMAnd the thermal history of the IGM

Tom TheunsInstitute for Computational Cosmology, Durham, UKDepartment of Physics, Antwerp, Belgium

Page 2: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

The intergalactic medium can be observed in absorption towards distant bright sources (QSOs, GRBs)

Page 3: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

UVES+VLT and HiRes+Keck have revolutionised these data in terms of S/N and resolution

Page 4: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

The filamentary pattern of the cosmic web produces absorption lines very similar to those seen in QSO spectra.

Cen & Ostriker ‘94Gas density contours in a cosmological box of size 4Mpc

Hubble volume simulation

Page 5: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Increased CPU power has made the simulations more realistic

Simulated versus observed high-resolution spectrum.Which is which?

Page 6: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Voigt profile fits can be used to characterise the statistics of lines

Page 7: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

The evolution of the column-density fits well with observations for an ionising background dominated by QSOs

Page 8: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Other flux statistics fit well as too.

Flux PDF Flux PS

Page 9: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Simulations with feedback produce metal lines not unlike the observed ones, without drastically altering the HI lines

Page 10: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

shocked gas unshocked, photo-ionised gas

Most of the volume is filled with warm photo-ionised gas, with shocks occupying a small volume around haloes and large filaments

Page 11: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

When the IGM is highly ionised, the (photo)-heating rate becomes small.

Page 12: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Page 13: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Photo-ionisation heating produces a well-defined -T relation in the low-density IGM that produces the Ly-forest. (Hui & Gnedin 1997)

Temperature of the IGM

Page 14: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Page 15: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

The IGM temperature affects the widths of the Lyman- lines

TT, Schaye & Haehnelt

Page 16: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Line-width (b) and temperature are relatedColumn-density (NH) and density are relatedHence can determine -T relation

Schaye et al, Ricotti et al, McDonald et al

Page 17: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

IGM temperature as function of redshift.

Schaye et al.

Page 18: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Photo-heating rate is less than adiabatic cooling rate

Page 19: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

If no other heat sources, HI reionization late?

Theuns et al.

Page 20: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

(Perceived?) Tension: zreion=17 (WMAP) or zreion around 6 (quasars)?

Page 21: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Tom Abel

Ciardi et al.

Page 22: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Wavelets are also sensitive to line-widths

Theuns & Zaroubi

Page 23: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Observed QSO looks similar to simulation with HeII reionisation, but without evidence for T fluctuations.

Theuns et al.Zaldarriaga.

Page 24: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

IGM temperature also affects optical depth (because recombination rate depends on T)

Page 25: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

Sloan DA too noisy to see anything?

Bernardi et al.

Page 26: Tom Theuns Institute for Computational Cosmology, Durham, UK Department of Physics, Antwerp, Belgium Munich 2005 Reionization And the thermal history of

Tom Theuns: IGM thermal history

To do list:

better constrain T evolution better constrain fluctuations

other heating sources? (cosmic rays? X-rays? dust?)

Thank you.