1992
DOI: 10.1093/mnras/255.2.319
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The Gunn-Peterson effect and the H I column density distribution of Lyman alpha forest clouds at z = 4

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Cited by 44 publications
(36 citation statements)
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“…Jenkins & Ostriker (1991) and Webb et al (1992), acknowledging this problem, attempted to model the pixel intensity distribution with continuum absorption and variable contributions from discrete lines. Their results show that τ GP can be produced both ways, by blending of weak lines below the detection threshold or by a constant pedestal of absorption.…”
Section: Lyman Alpha Clouds Confined By the Pressure Of An Intercloudmentioning
confidence: 99%
“…Jenkins & Ostriker (1991) and Webb et al (1992), acknowledging this problem, attempted to model the pixel intensity distribution with continuum absorption and variable contributions from discrete lines. Their results show that τ GP can be produced both ways, by blending of weak lines below the detection threshold or by a constant pedestal of absorption.…”
Section: Lyman Alpha Clouds Confined By the Pressure Of An Intercloudmentioning
confidence: 99%
“…The extent to which this eect is important depends on the shape of the ionizing spectrum and its evolution, neither of which are well quantied. The lack of a detectable Gunn-Peterson Lyman-absorption trough in the spectra high-redshift QSO's (Steidel & Sargent 1987;Webb et al 1992) suggests the IGM is highly ionized. The ionizing radiation eld estimated from the proximity eect (J 10 21 erg cm 2 s 1 Hz 1 ; Lu et al 1991) appears sucient t o prevent the gas from cooling in halos of velocity dispersion less than 35km s 1 until z 1.…”
Section: Coolingmentioning
confidence: 99%
“…The idea is to view a Lya forest spectrum as a random stochastic process (Press et al 1993). Every point in the spectrum is a random variable, e ¹t , drawn from the transmission probability density function f l ðe ¹t Þ, also known as flux decrement distribution function (Kim et al 1997;Rauch et al 1997) or distribution of intensities (Jenkins & Ostriker 1991;Webb et al 1992). In principle, we have a different probability density function at each wavelength such that, for example, the moments of f l are functions of wavelength.…”
Section: T E C H N I Q U Ementioning
confidence: 99%
“…We can define an effective optical depth, t eff , as a function of observed wavelength, l, by e ¹t eff ðlÞ ϵ he ¹tðlÞ i: ð1Þ In the following we will neglect any contribution to t eff from the classical Gunn-Peterson effect which is limited to t GP Շ 0:04 (Webb et al 1992 …”
Section: The Mean Lya Transmissionmentioning
confidence: 99%