An Analytic Formulation of 21-cm Signal from Early Phase of Epoch of Reionization

We present an analytic formulation to model the fluctuating component of the HI signal from the epoch of reionization during the phase of partial heating. During this phase, we assume self-ionized regions, whose size distribution can be computed using excursion set formalism, to be surrounded by heated regions. We model the evolution of heating profile around these regions (near zone) and their merger into the time-dependent background (far zone). We develop a formalism to compute the two-point correlation function for this topology, taking into account the heating auto-correlation and heating-ionization cross-correlation. We model the ionization and X-ray heating using four parameters: efficiency of ionization, $\zeta$, number of X-ray photons per stellar baryon, $N_{\rm heat}$, the spectral index of X-ray photons, $\alpha$, and the minimum frequency of X-ray photons, $\nu_{\rm min}$. We compute the HI signal in the redshift range $10 < z < 20$ for the $\Lambda$CDM model for a set of these parameters. We show that the HI signal for a range of scales $1\hbox{-}8 \, \rm Mpc$ show a peak strength $100\hbox{-}1000 \, \rm (mK)^2$ during the partially heated era. The redshift at which the signal makes a transition to uniformly heated universe depends on modelling parameters, e.g. if $\nu_{\rm min}$ is changed from $100 \, \rm eV$ to $1 \, \rm keV$, this transition moves from $z \simeq 15$ to $z \simeq 12$. This result, along with the dependence of the HI signal on modelling parameters, is in reasonable agreement with existing results from N-body simulations.Comment: 35 pages, 17 figures, published in Ap

Analytic Formulation of 21 cm Signal from Cosmic Dawn: Lyα\alpha Fluctuations

We present an analytic formalism to compute the fluctuating component of the \ion{H}{1} signal and extend it to take into account the effects of partial Lyman-$\alpha$ coupling during the era of cosmic dawn. We use excursion set formalism to calculate the size distribution of randomly distributed self-ionized regions. These ionization bubbles are surrounded by partially heated and Lyman-$\alpha$ coupled regions, which create spin temperature $T_S$ fluctuations. We use the ratio of number of Lyman-$\alpha$ to ionizing photon ($f_L$) and number of X-ray photons emitted per stellar baryons ($N_{\rm heat}$) as modeling parameters. Using our formalism, we compute the global \ion{H}{1} signal, its auto-correlation and power spectrum in the redshift range $10 \le z \le 30$ for the $\Lambda$CDM model. We check the validity of this formalism for various limits and simplified cases. Our results agree reasonably well with existing results from N-body simulations, in spite of following a different approach and requiring orders of magnitude less computation power and time. We further apply our formalism to study the fluctuating component corresponding to the recent EDGES observation that shows an unexpectedly deep absorption trough in global \ion{H}{1} signal in the redshift range $15 <z< 19$. We show that, generically, the EDGES observation predicts larger signal in this redshift range but smaller signal at higher redshifts. We also explore the possibility of negative real-space auto-correlation of spin temperature and show it can be achieved for partial Lyman-$\alpha$ coupling in many cases corresponding to simplified models and complete model without density perturbations.Comment: Comments and suggestions are welcome. arXiv admin note: text overlap with arXiv:1711.0382

Primordial Magnetic Fields in the Post-recombination Era and Early Reionization

We explore the ways in which primordial magnetic fields influence the thermal and ionization history of the post-recombination universe. After recombination the universe becomes mostly neutral resulting also in a sharp drop in the radiative viscosity. Primordial magnetic fields can then dissipate their energy into the intergalactic medium (IGM) via ambipolar diffusion and, for small enough scales, by generating decaying MHD turbulence. These processes can significantly modify the thermal and ionization history of the post-recombination universe. We show that the dissipation effects of magnetic fields which redshifts to a present value $B_{0}=3\times 10^{-9}$ Gauss smoothed on the magnetic Jeans scale and below, can give rise to Thomson scattering optical depths \tau \ga 0.1, although not in the range of redshifts needed to explain the recent WMAP polarization observations. We also study the possibility that primordial fields could induce the formation of subgalactic structures for z \ga 15. We show that early structure formation induced by nano-Gauss magnetic fields is potentially capable of producing the early re-ionization implied by the WMAP data. Future CMB observations will be very useful to probe the modified ionization histories produced by primordial magnetic field evolution and constrain their strength.Comment: 19 pages, 7 figures, Minor changes to match version accepted in MNRA

Galactic dust polarized emission at high latitudes and CMB polarization

We estimate the dust polarized emission in our galaxy at high galactic latitudes, which is the dominant foreground for measuring CMB polarization using the high frequency instrument (HFI) aboard Planck surveyor. We compare it with the level of CMB polarization and conclude that, for angular scales $\le 1^{\circ}$, the scalar-induced CMB polarization and temperature-polarization cross-correlation are much larger than the foreground level at $\nu \simeq 100 GHz$. The tensor-induced signals seem to be at best comparable to the foreground level.}Comment: Latex document, 4 pages, 2 figures, to appear in "Fundamental parameters in Cosmology", Rencontres de Moriond, 199