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arXiv · 2608.07817

Overview and status of BICEP Array's BA4-90/150 CMB polarimeter

M. A. Petroff·P. A. R. Ade·Z. Ahmed·M. Amiri·D. Barkats·R. Basu Thakur·C. A. Bischoff·D. Beck·J. J. Bock·V. Buza·B. Cantrall·J. R. Cheshire IV·J. Connors·J. Cornelison·M. Crumrine·A. J. Cukierman·E. Denison·L. Duband·M. A. Echter·M. Eiben·B. D. Elwood·S. Fatigoni·J. P. Filippini·A. Fortes·M. Gao·C. Giannakopoulos·N. Goeckner-Wald·D. C. Goldfinger·S. Gratton·J. A. Grayson·A. Greathouse·P. K. Grimes·M. Halpern·S. Henderson·T. D. Hoang·J. Hubmayr·H. Hui·K. D. Irwin·M. Izquierdo Poza·J. H. Kang·K. S. Karkare·S. Kefeli·J. M. Kovac·C. Kuo·K. Lasko·K. Lau·M. Lautzenhiser·T. Liu·S. C. Mackey·N. Maher·K. G. Megerian·L. Minutolo·L. Moncelsi·Y. Nakato·H. T. Nguyen·R. O'Brient·S. N. Paine·A. Patel·A. R. Polish·T. Prouve·C. Pryke·C. D. Reintsema·T. Romand·M. Salatino·A. Schillaci·B. Schmitt·B. Singari·A. Soliman·T. St. Germaine·A. Steiger·B. Steinbach·R. Sudiwala·K. L. Thompson·C. Tucker·A. D. Turner·C. Vergès·A. G. Vieregg·A. Wandui·A. C. Weber·J. Willmert·W. L. K. Wu·H. Yang·C. Yu·L. Zeng·C. Zhang·S. Zhang
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Abstract

The inflation paradigm postulates a period of rapid expansion in the early Universe, which would generate gravitational waves. These tensor perturbations would produce a faint B-mode signature in the polarization of the cosmic microwave background (CMB), but this signal is orders of magnitude weaker than that from the CMB's other anisotropy and that from astrophysical foregrounds. Placing more-stringent upper limits on this signal or making a definitive detection thus requires exceptional control over instrument and measurement systematics, in addition to extremely-deep maps. The fourth BICEP Array receiver, BA4-90/150, aims to build and improve upon the heritage of the field-leading BICEP series of small-aperture CMB experiments with a dichroic instrument observing in 90 and 150 GHz bands, to advance the search for the inflationary B-mode signal. The instrument will utilize transition-edge-sensor bolometers, which will be read out using a new two-level time-division-multiplexed system and be fed via feedhorn-coupled orthomode transducers and refined cold refractive optics, with the goal of both improving systematics control and sensitivity over existing receivers. With a planned deployment to the South Pole in the 2026-27 austral summer, the instrument will occupy the fourth and final remaining slot in the BICEP Array mount, completing the phaseout of Keck Array receivers. An overview of the BA4-90/150 receiver will be presented, along with a discussion of its current status and future plans for the instrument.

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M. A. Petroff, P. A. R. Ade, Z. Ahmed, M. Amiri, D. Barkats, R. Basu Thakur, C. A. Bischoff, D. Beck, J. J. Bock, V. Buza, B. Cantrall, J. R. Cheshire IV, J. Connors, J. Cornelison, M. Crumrine, A. J. Cukierman, E. Denison, L. Duband, M. A. Echter, M. Eiben, B. D. Elwood, S. Fatigoni, J. P. Filippini, A. Fortes, M. Gao, C. Giannakopoulos, N. Goeckner-Wald, D. C. Goldfinger, S. Gratton, J. A. Grayson, A. Greathouse, P. K. Grimes, M. Halpern, S. Henderson, T. D. Hoang, J. Hubmayr, H. Hui, K. D. Irwin, M. Izquierdo Poza, J. H. Kang, K. S. Karkare, S. Kefeli, J. M. Kovac, C. Kuo, K. Lasko, K. Lau, M. Lautzenhiser, T. Liu, S. C. Mackey, N. Maher, K. G. Megerian, L. Minutolo, L. Moncelsi, Y. Nakato, H. T. Nguyen, R. O'Brient, S. N. Paine, A. Patel, A. R. Polish, T. Prouve, C. Pryke, C. D. Reintsema, T. Romand, M. Salatino, A. Schillaci, B. Schmitt, B. Singari, A. Soliman, T. St. Germaine, A. Steiger, B. Steinbach, R. Sudiwala, K. L. Thompson, C. Tucker, A. D. Turner, C. Vergès, A. G. Vieregg, A. Wandui, A. C. Weber, J. Willmert, W. L. K. Wu, H. Yang, C. Yu, L. Zeng, C. Zhang, S. Zhang. 2026-08-07. Overview and status of BICEP Array's BA4-90/150 CMB polarimeter. https://arxiv.org/abs/2608.07817

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