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Status of DMRadio-50L and DMRadio-m$^3$
by Nicholas M. Rapidis
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Submission summary
Authors (as registered SciPost users): | Nicholas Marcos Rapidis |
Submission information | |
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Preprint Link: | https://arxiv.org/abs/2210.07215v2 (pdf) |
Date accepted: | 2023-04-24 |
Date submitted: | 2022-11-09 19:26 |
Submitted by: | Rapidis, Nicholas Marcos |
Submitted to: | SciPost Physics Proceedings |
Proceedings issue: | 14th International Conference on Identification of Dark Matter (IDM2022) |
Ontological classification | |
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Academic field: | Physics |
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Approach: | Experimental |
Abstract
Recent theoretical advancements have made the QCD axion a stronger dark matter candidate, especially in the sub-$\mu\text{eV}$ range. While cavity haloscopes have made significant progress in excluding QCD axions in the $1 - 100\ \mu\text{eV}$ region, the $1 \text{ peV} - 1\ \mu\text{eV}$ region remains unexplored. The DMRadio program consists of a series of experiments designed to probe low mass axions. DMRadio-50L uses a 1 T average field toroidal magnet and a high-Q LC-oscillator with target sensitivity to axions of $g_{a\gamma\gamma} <5\times10^{-15}\text{ GeV}^{-1}$ between 5 kHz and 5 MHz. DMRadio-m$^3$ consists of a higher frequency LC-oscillator in a 4 T peak field solenoidal magnet with sensitivity to the DFSZ model of QCD axions between 30 MHz and 200 MHz. In this work, we present the status of DMRadio-50L and DMRadio-m$^3$.
List of changes
We have edited the manuscript based off of the referee's recommendations:
- Caption for figure 1 includes descriptions of other limits.
- We clarify our approach of using the standard halo model to set sensitivity limits but are also considering other models in our analysis.
-We have addressed the repeated use of a phrase in the manuscript.
We have also updated citation [35] to include the arXiv identifier.
Published as SciPost Phys. Proc. 12, 036 (2023)