EOR Detection Strategies Somnath Bharadwaj IIT Kharagpur
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Will be seen in Emission T s > T Varies with angle and frequency Fluctuations caused by: Variations in the neutral fraction Fluctuations in gas density (Dark Matter Fluctuations) Peculiar Velocities The 21-cm EOR Signal yy xx
Radio Interferometric Arrays Frequency MHz z GMRT 30 antennas 45m diameter
The 21-cm Signal yy xx z
Interferometry and Visibilities / d A visibility V(U, ) records a single Fourier component of I( with angular wave number 2 U Angular multi-pole
Baseline Distribution U Visibility V(U, ) 21-cm Signal Noise (inherent to the observation) Foregrounds from other astrophysical Sources Man-made RFI
Why bother about Visibilities? FT Why not try to detect the signal in the Image? Noise in different visibilities is uncorrelated Noise in different pixels of the image is correlated Imaging Artifacts Incomplete u-v coverage
The w term l = cos m = cos
Small Field of View FT DD
Relative Contributions
2 Easy Ways Statistical Detection Statistical properties of the 21-cm signal are significantly different from those of foregrounds and noise. Use this to separate out the signal. Ionized Bubble Detection Develop a template based on prior knowledge of the expected signal. Use this to search for the signal buried in noise and foregrounds. Matched Filter.
Statistical Detection Multi-frequency angular power spectrum Jy 2 K2K2
Visibility correlations
The Estimator U1U1 U2U2 D/ V 2 (U, ) U < D/ U >> U Self Correlations avoided 0 ~ D
Begum, A. et al MNRAS, 372, L pc 80 pc
The HI Signal Bharadwaj, S.& Sethi, S.K. 2001, 22, 293 Morales, M. F. & Hewitt, J. 2004, ApJ, 615,7; Bharadwaj, S. & Ali, Sk.S., 2005, MNRAS,356, Jy 2
Decorrelation
14 hrs GMRT Observations RA DEC MHz Observation 5 MHz Bandwidth 62.5 kHz resolution Primary Beam FWHM ~4 deg. Synthesized beam 28” x 23” Noise 1.6 mJy/Beam Ali, Sk. S. et al. 2008, MNRAS, 385, 2166
Visibility Correlations
Foregrounds Santos, M.J. et al. 2005, ApJ,625,575; Di Matteo, T. et al., 2002,ApJ, 564,576 Zaldarriaga, M. et al., 2004, ApJ, 608, 622
Foreground Removal Foregrounds are all continuum sources Emissions at ~1 MHz are expected to be highly correlated The HI signal decorrelates within 1 MHz In the image cube – fit and subtract a smooth polynomial in along each pixel Jelic, V. et al. 2008, MNRAS, 389, 1319 Bowman, J. D. et al. 2009, ApJ, 695, 183
Foreground Removal Advantages in working with visibilities Grid the visibilities V(U, - 3D grid Fit and subtract a smooth polynomial along at each U grid point Liu, A. 2009, arxiv McQuinn, M. et al. 2006, ApJ, 653,815; Morales, M.F. et al. 2006, ApJ,648, 767
Foreground Removal The foreground contributions to V 2 (U, ) is predicted to decorrelate less than 1% in the 5 MHz bandwidth of our observation The signal contribution decorrelates within 1 MHz Fit V 2 (U, ) with a smooth polynomial in and subtract this out
Measured Decorrelations
Three Visibility Correlation Probes the Bispectrum Significant as the HI distribution at reionization is expected to be quite non- Gaussian Non-zero only if three baselines form a closed triangle Decorrelates within Bharadwaj, S. & Pandey, S.K. 2005, MNRAS, 358, 968
Ionized Bubble Detection Datta, K.K. et al., 2007, MNRAS, 382, 809
Signal from an HII bubble 70 Jy Bubble at center of field of view, phase factor and fall in amplitude if shifted
The Problem of Signal Detection
The Contaminants We treat the Noise, Foregrounds and the HI Fluctuations outside the bubble as independent random signals V(U, )=S(U, ) + N(U, ) + F(U, ) + H(U, )
Matched Filter V(U, )=S(U, ) + N(U, ) + F(U, ) + H(U, )
The Variance Dominated by Foregrounds Exceeds the Signal Foreground Removal necessary
The Filter Remove Foregrounds Optimize Signal to Noise Ratio
Predictions Depends on antennas and baseline coverage Filter effectively removes foreground Noise reduces with observing time HI fluctuations outside the bubble impose a fundamental restriction on the smallest bubble that can be detected x HI =1 Z= hrs, > 22 Mpc
2 Easy Ways to Detect the EOR 21-cm Signal
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