The real-time data processing and acquisition system for Project 8 Phase II
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| Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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| Formato: | Preprint |
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2025
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| author | Esfahani, A. Ashtari Banducci, A. Böser, S. Buzinsky, N. Cervantes, R. Claessens, C. de Viveiros, L. Fertl, M. Formaggio, J. A. Gladstone, L. Grando, M. Guigue, M. Hartse, J. Heeger, K. M. Jones, A. M. Kazkaz, K. LaRoque, B. H. Lindman, A. Monreal, B. Nikkel, J. A. Novitski, E. Oblath, N. S. Pettus, W. Robertson, R. G. H. Rybka, G. Saldaña, L. Slocum, P. L. Sun, Y. -H. Surukuchi, P. T. Telles, A. B. Thomas, F. Thomas, M. Thümmler, T. Tvrznikova, L. VanDevender, B. A. Weiss, T. E. Young, A. Zayas, E. Ziegler, A. |
| author_facet | Esfahani, A. Ashtari Banducci, A. Böser, S. Buzinsky, N. Cervantes, R. Claessens, C. de Viveiros, L. Fertl, M. Formaggio, J. A. Gladstone, L. Grando, M. Guigue, M. Hartse, J. Heeger, K. M. Jones, A. M. Kazkaz, K. LaRoque, B. H. Lindman, A. Monreal, B. Nikkel, J. A. Novitski, E. Oblath, N. S. Pettus, W. Robertson, R. G. H. Rybka, G. Saldaña, L. Slocum, P. L. Sun, Y. -H. Surukuchi, P. T. Telles, A. B. Thomas, F. Thomas, M. Thümmler, T. Tvrznikova, L. VanDevender, B. A. Weiss, T. E. Young, A. Zayas, E. Ziegler, A. |
| contents | In Phase II of the Project 8 neutrino mass experiment, electrons from the decays of tritium or ${}^{83\mathrm{m}}$Kr are detected via their $\approx$26 GHz cyclotron radiation while contained within a circular waveguide. The signal from a given electron is characterized as a brief chirp, lasting $\lesssim$10 ms and changing in frequency by $\lesssim$1 MHz/ms. To detect these signals, the Project 8 collaboration developed a data acquisition (DAQ) system tailored to the signal properties. The DAQ is responsible for simultaneously selecting up to three 100 MHz-wide frequency windows to study, detect, and trigger on likely signals from different electron kinetic energies, and for writing the relevant data to disk. We describe the Phase II DAQ system in detail and address how the system was used for data-taking operations. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2506_22392 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | The real-time data processing and acquisition system for Project 8 Phase II Esfahani, A. Ashtari Banducci, A. Böser, S. Buzinsky, N. Cervantes, R. Claessens, C. de Viveiros, L. Fertl, M. Formaggio, J. A. Gladstone, L. Grando, M. Guigue, M. Hartse, J. Heeger, K. M. Jones, A. M. Kazkaz, K. LaRoque, B. H. Lindman, A. Monreal, B. Nikkel, J. A. Novitski, E. Oblath, N. S. Pettus, W. Robertson, R. G. H. Rybka, G. Saldaña, L. Slocum, P. L. Sun, Y. -H. Surukuchi, P. T. Telles, A. B. Thomas, F. Thomas, M. Thümmler, T. Tvrznikova, L. VanDevender, B. A. Weiss, T. E. Young, A. Zayas, E. Ziegler, A. Instrumentation and Detectors In Phase II of the Project 8 neutrino mass experiment, electrons from the decays of tritium or ${}^{83\mathrm{m}}$Kr are detected via their $\approx$26 GHz cyclotron radiation while contained within a circular waveguide. The signal from a given electron is characterized as a brief chirp, lasting $\lesssim$10 ms and changing in frequency by $\lesssim$1 MHz/ms. To detect these signals, the Project 8 collaboration developed a data acquisition (DAQ) system tailored to the signal properties. The DAQ is responsible for simultaneously selecting up to three 100 MHz-wide frequency windows to study, detect, and trigger on likely signals from different electron kinetic energies, and for writing the relevant data to disk. We describe the Phase II DAQ system in detail and address how the system was used for data-taking operations. |
| title | The real-time data processing and acquisition system for Project 8 Phase II |
| topic | Instrumentation and Detectors |
| url | https://arxiv.org/abs/2506.22392 |