An efficient phase-shifting scheme for bolometric additive interferometry

TL;DR

This paper proposes an optimized phase-shifting scheme for bolometric interferometry that enhances sensitivity to CMB polarization signals, making it competitive with direct imaging methods.

Contribution

It introduces a coherent summation phase-shifting scheme that maximizes signal-to-noise ratio in bolometric interferometers for CMB polarization measurements.

Findings

Maximized SNR with coherent summation of equivalent baselines.

Bolometric interferometer competitiveness with imagers of same horn count.

Monte-Carlo simulations confirm the theoretical results.

Abstract

Context: Most upcoming CMB polarization experiments will use direct imaging to search for the primordial gravitational waves through the B-modes. Bolometric interferometry is an appealing alternative to direct imaging that combines the advantages of interferometry in terms of systematic effects handling and those of bolometric detectors in terms of sensitivity. Aims: We calculate the signal from a bolometric interferometer in order to investigate its sensitivity to the Stokes parameters paying particular attention to the choice of the phase-shifting scheme applied to the input channels in order to modulate the signal. Methods: The signal is expressed as a linear combination of the Stokes parameter visibilities whose coefficients are functions of the phase-shifts. Results: We show that the signal to noise ratio on the reconstructed visibilities can be maximized provided the fact that the phase-shifting scheme is chosen in a particular way called coherent summation of equivalent baselines. As a result, a bolometric interferometer is competitive with an imager having the same number of horns, but only if the coherent summation of equivalent baselines is performed. We confirm our calculations using a Monte-Carlo simulation. We also discuss the impact of the uncertainties on the relative calibration between bolometers and propose a way to avoid this systematic effect.