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How exactly did the universe become neutral

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In this article, the authors presented a treatment of H, He I, and He II recombination in the early universe, using multilevel atoms and evolving the population of each level with redshift by including all bound-bound and bound-free transitions.
Abstract
We present a re—ned treatment of H, He I, and He II recombination in the early universe. The diUer- ence from previous calculations is that we use multilevel atoms and evolve the population of each level with redshift by including all bound-bound and bound-free transitions. In this framework we follow several hundred atomic energy levels for H, He I, and He II combined. The main improvements of this method over previous recombination calculations are (1) allowing excited atomic level populations to depart from an equilibrium distribution, (2) replacing the total recombination coefficient with recombi- nation to and photoionization from each level calculated directly at each redshift step, and (3) correct treatment of the He I atom, including the triplet and singlet states. We —nd that is approximately 10% smaller at redshifts than in previous calcu- x e (4 n e /n H ) (800 lations, as a result of the nonequilibrium of the excited states of H that is caused by the strong but cool radiation —eld at those redshifts. In addition, we —nd that He I recombination is delayed compared with previous calculations and occurs only just before H recombination. These changes in turn can aUect the predicted power spectrum of microwave anisotropies at the few percent level. Other improvements, such as including molecular and ionic species of H, including complete heating and cooling terms for the evolution of the matter temperature, including collisional rates, and including feedback of the secondary spectral distortions on the radiation —eld, produce negligible change to the ionization fraction. The lower at low z found in this work aUects the abundances of H molecular and ionic species by 10%¨25%. x e However, this diUerence is probably not larger than other uncertainties in the reaction rates. Subject headings: atomic processescosmic microwave backgroundcosmology: theory ¨ early universe

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Citations
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Planck 2015 results - XIII. Cosmological parameters

Peter A. R. Ade, +337 more
TL;DR: In this article, the authors present a cosmological analysis based on full-mission Planck observations of temperature and polarization anisotropies of the cosmic microwave background (CMB) radiation.
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Planck 2013 results. XVI. Cosmological parameters

Peter A. R. Ade, +327 more
TL;DR: In this paper, the authors present the first cosmological results based on Planck measurements of the cosmic microwave background (CMB) temperature and lensing-potential power spectra, which are extremely well described by the standard spatially-flat six-parameter ΛCDM cosmology with a power-law spectrum of adiabatic scalar perturbations.
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Planck 2018 results. VI. Cosmological parameters

Nabila Aghanim, +232 more
TL;DR: In this article, the authors present cosmological parameter results from the full-mission Planck measurements of the cosmic microwave background (CMB) anisotropies, combining information from the temperature and polarization maps and the lensing reconstruction.
References
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Book

Principles of Physical Cosmology

TL;DR: Peebles as mentioned in this paper provides a comprehensive overview of today's physical cosmology, including the history of the discovery of the expanding universe, and discusses the most notable recent attempts to understand the origin and structure of the universe.
Journal ArticleDOI

A Measurement of excess antenna temperature at 4080-Mc/s

TL;DR: In this paper, the effective zenith noise temperature of the 20-foot horn-reflector antenna (Crawford, Hogg, and Hunt 1961) at the Crawford Hill Laboratory, Holmdel, New Jersey, at 4080 Mc/s has yielded a value about 3.5 K higher than expected.
Journal ArticleDOI

The Cosmic Microwave Background spectrum from the full COBE FIRAS data set

TL;DR: In this article, the Far-InfraRed Absolute Spectrophotometer (FIRAS) on board the COBE (COsmic Background Explorer) is used to measure the difference between the cosmic microwave background and a precise blackbody spectrum.
Journal ArticleDOI

Recombination-line intensities for hydrogenic ions – I. Case B calculations for H I and He II

TL;DR: In this paper, the relative intensities of H I and He II recombination lines were determined for a larger range of temperature and density than previously considered and with the upper principle quantum number up to 50 and the lower one up to 29.
Journal ArticleDOI

How small were the first cosmological objects

TL;DR: In this article, the minimum mass that a virialized gas cloud must have in order to be able to cool in a Hubble time is computed, using a detailed treatment of the chemistry of molecular hydrogen.
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