We calculate the contribution to the ultraviolet background (UVB) from thermal emission from gas shock heated during cosmic structure formation. Our main calculation is based on an updated version of Press–Schechter theory. It is consistent with a more empirical estimate based on the observed properties of galaxies and the observed cosmic star formation history. Thermal UVB emission is characterized by a hard spectrum extending well beyond 4 Ryd. The bulk of the radiation is produced by objects in the mass range 1011–1013 M⊙, i.e. large galaxies and small groups. We compute a composite UVB spectrum due to quasi-stellar object (QSO), stellar and thermal components. The ratio of the UVB intensities at the H and He Lyman limits increases from 60 at z = 2 to more than 300 at z = 6. A comparison of the resulting photoionization rates to the observed Gunn–Peterson effect at high redshifts constrains the escape fraction of ionizing photons from galaxies to be less than a few per cent. Near 1 Ryd, thermal and stellar emission are comparable, amounting to about 10, 20 and 35 per cent of the total flux at redshifts of 3, 4.5 and higher, respectively. However, near the ionization threshold for He ii, the thermal contribution is much stronger. It is comparable to the QSO intensity already at redshift ∼3 and dominates at redshifts above 4. Thermal photons alone are enough to produce and sustain He ii reionization already at z≈ 6. We discuss the possible implications of our results for the thermal history of the intergalactic medium, in particular for He ii reionization.

Ultraviolet background radiation from cosmic structure formation

FERRARA, ANDREA;
2004

Abstract

We calculate the contribution to the ultraviolet background (UVB) from thermal emission from gas shock heated during cosmic structure formation. Our main calculation is based on an updated version of Press–Schechter theory. It is consistent with a more empirical estimate based on the observed properties of galaxies and the observed cosmic star formation history. Thermal UVB emission is characterized by a hard spectrum extending well beyond 4 Ryd. The bulk of the radiation is produced by objects in the mass range 1011–1013 M⊙, i.e. large galaxies and small groups. We compute a composite UVB spectrum due to quasi-stellar object (QSO), stellar and thermal components. The ratio of the UVB intensities at the H and He Lyman limits increases from 60 at z = 2 to more than 300 at z = 6. A comparison of the resulting photoionization rates to the observed Gunn–Peterson effect at high redshifts constrains the escape fraction of ionizing photons from galaxies to be less than a few per cent. Near 1 Ryd, thermal and stellar emission are comparable, amounting to about 10, 20 and 35 per cent of the total flux at redshifts of 3, 4.5 and higher, respectively. However, near the ionization threshold for He ii, the thermal contribution is much stronger. It is comparable to the QSO intensity already at redshift ∼3 and dominates at redshifts above 4. Thermal photons alone are enough to produce and sustain He ii reionization already at z≈ 6. We discuss the possible implications of our results for the thermal history of the intergalactic medium, in particular for He ii reionization.
2004
Settore FIS/05 - Astronomia e Astrofisica
Settore PHYS-05/A - Astrofisica, cosmologia e scienza dello spazio
radiation mechanisms: thermal; shock waves; large-scale structure of Universe
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11384/6025
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