Volume 399, Issue 1 pp. L132-L136

The optimal redshift for detecting ionized bubbles in H i 21-cm maps

Kanan K. Datta

Corresponding Author

Kanan K. Datta

Department of Physics and Meteorology & Centre for Theoretical Studies, IIT, Kharagpur 721302, India

E-mail: [email protected] (KKD); [email protected] (SB); [email protected] (TRC)Search for more papers by this author
Somnath Bharadwaj

Corresponding Author

Somnath Bharadwaj

Department of Physics and Meteorology & Centre for Theoretical Studies, IIT, Kharagpur 721302, India

E-mail: [email protected] (KKD); [email protected] (SB); [email protected] (TRC)Search for more papers by this author
T. Roy Choudhury

Corresponding Author

T. Roy Choudhury

Harish-Chandra Research Institute, Chhatnag Road, Jhusi, Allahabad 211019, India

E-mail: [email protected] (KKD); [email protected] (SB); [email protected] (TRC)Search for more papers by this author
First published: 01 October 2009
Citations: 3

ABSTRACT

The detection of individual ionized bubbles in H i 21-cm maps is one of the most promising, direct probes of the epoch of reionization (EoR). At least 1000 h of observation would be required for such a detection with either the currently functioning Giant Metrewave Radio Telescope (GMRT) or the upcoming Murchison Widefield Array (MWA). Considering the large investment for telescope time, it is essential to identify the ‘optimal redshift’ where the prospects of a detection are most favourable. We find that the optimal redshift is determined by a combination of instrument dependent factors and the evolution of the neutral fraction xH i. We find that the redshift range 8.1 ± 1.1 and 9.8 ± 1 are optimum for detecting ionized bubbles with the GMRT and MWA, respectively. The prospects of a detection, we find, are more favourable in a scenario with late reionization with xH i≈ 0.5 at z≈ 7.5 as compared to an early reionization model where xH i≈ 0.5 at z≈ 10. In the late reionization scenario, for both instruments a detection is possible for bubbles of comoving radius Rb≥ 30 Mpc with 1000 h of observation. Future observations will either lead to the detection of ionized bubbles, or in the event of non-detection, lead to constraints on the product xH iRγb for the observational volume, where γ= 1.5 and 2 for GMRT and MWA, respectively.

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