- Main
Electromagnetic modeling and science reach of DMRadio-m3
- AlShirawi, A;
- Ankel, V;
- Bartram, C;
- Begin, J;
- Bell, C;
- Benabou, JN;
- Brouwer, L;
- Chaudhuri, S;
- Cho, H-M;
- Corbin, J;
- Craddock, W;
- Cuadra, S;
- Droster, A;
- Echevers, J;
- Foster, JW;
- Fry, JT;
- Graham, PW;
- Henning, R;
- Irwin, KD;
- Kadribasic, F;
- Kahn, Y;
- Keller, A;
- Kolevatov, R;
- Kuenstner, S;
- Kunder, A;
- Kurita, N;
- Leder, AF;
- Li, D;
- Otto, N;
- Ouellet, JL;
- Pappas, KMW;
- Phipps, A;
- Rapidis, NM;
- Safdi, BR;
- Salemi, CP;
- Simanovskaia, M;
- Singh, J;
- Stark, P;
- van Assendelft, EC;
- van Bibber, K;
- Wells, K;
- Wiedemann, J;
- Winslow, L;
- Wisniewski, WJ;
- Wright, D;
- Yi, AK;
- Young, BA
Published Web Location
https://doi.org/10.1103/bwgd-kxsbAbstract
is an experimental search for dark matter axions. It uses a solenoidal dc magnetic field to convert an axion dark-matter signal to an ac electromagnetic response in a coaxial copper pickup. The current induced by this axion signal is measured by dc SQUIDs. is designed to be sensitive to Kim-Shifman-Vainshtein-Zakharov (KSVZ) and Dine-Fischler-Srednicki-Zhitnisky (DFSZ) QCD axion models in the 10–200 MHz ( ) range, and to axions with over 5–30 MHz as an extended goal. In this work, we present the electromagnetic modeling of the response of the experiment to an axion signal over the full frequency range of , which extends from the low-frequency, lumped-element limit to a regime where the axion Compton wavelength is only a factor of 2 larger than the detector size. With these results, we determine the live time and sensitivity of the experiment. The primary science goal of sensitivity to DFSZ axions across 30–200 MHz can be achieved with a live scan time of 2.9 years.
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