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Spectroscopy of the Double Quasars Q1343+266AB: I. a New Determination of the Size of Lyman-Alpha Forest Absorbers
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abstract
We have obtained spectroscopy of Q 1343+266 AB, a pair of quasars at redshift z = 2.03 with a projected separation of 9.5 arcseconds. This system is well-suited for probing the Ly-alpha forest, since the two component spectra show several Ly-alpha lines in common and several others not. Using Bayesian statistics, under the idealization of uniform-radius spherical absorbers, we find that the Ly-alpha cloud radius at $z \approx 1.8$ lies in the range $40\hkpc < R < 280 \hkpc$ with $98\%$ confidence in a $(\Omega_o, \Lambda_o) = (1, 0)$ model universe, where $h =(H_o / 100 km s^{-1} Mpc^{-1})$. The median value of R is 90 h^-1 kpc. \ These numbers scale up by a factor 1.44 for $(\Omega_o, \Lambda_o) =(0.1, 0)$; and by a factor 1.85 for (0.1, 0.9). Pressure-confined and freely-expanding Ly-alpha cloud models in which the absorbers formed in a significantly more compressed state at $z \gg 2$ are contradicted by these new data, as are models involving stably-confined gas concentrations in photoionization equilibrium within minihalos of cold dark matter. The comoving density of Ly-alpha forest objects at $z\sim 2$ is $\sim 0.3 h (R/100 kpc)^{-2} Mpc^{-3}$ in a (1,0) model universe. This suggests a possible identification of Ly-alpha clouds with the unvirialized, collapsing progenitors of the faint, blue galaxies at $z\sim 1$.
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Cited by 1 Pith paper
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On the Origin of the Ly$\alpha$ Damping Wing in Galaxies at $8\le z \le 10$: Explorations using the NINJA Simulations
At z=8-10, the strongest JWST damped Lyα absorbers require neutral gas inside and around galaxies, and the NINJA models still underproduce them unless additional unresolved birth-cloud gas is invoked.
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