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[1-1]
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Single electron detection and spectroscopy via relativistic cyclotron radiation,
D.M. Asner et al.,
Phys. Rev. Lett. 114 (2015) 162501,
arXiv:1408.5362.
[Project8:2014ivu]
-
[2-1]
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The Project 8 Neutrino Mass Experiment,
A. Ashtari Esfahani et al.
(Project 8),
arXiv:2203.07349, 2022.
Snowmass 2021.
[Project8:2022wqh]
-
[2-2]
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Determining the neutrino mass with Cyclotron Radiation Emission Spectroscopy - Project 8,
Ali Ashtari Esfahani et al.,
J.Phys. G44 (2017) 054004,
arXiv:1703.02037.
[Project8:2017nal]
-
[2-3]
-
Project 8: Determining neutrino mass from tritium $\beta$ decay using a frequency-based method,
P.J. Doe et al.
(Project 8),
arXiv:1309.7093, 2013.
[Project8:2013trt]
-
[3-1]
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Tritium Beta Spectrum and Neutrino Mass Limit from Cyclotron Radiation Emission Spectroscopy,
A. Ashtari Esfahani et al.
(Project 8),
Phys.Rev.Lett. 131 (2023) 102502,
arXiv:2212.05048.
[Project8:2022hun]
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[4-1]
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Energy and momentum dependence of the soft-axion interaction rate,
Killian Bouzoud, Jacopo Ghiglieri, M. Laine, G. S. S. Sakoda,
JHEP 05 (2026) 034,
arXiv:2601.08221.
[Bouzoud:2026rur]
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[4-2]
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The real-time data processing and acquisition system for Project 8 Phase II,
A. Ashtari Esfahani et al.,
Nucl.Instrum.Meth.A 1081 (2026) 170843,
arXiv:2506.22392.
[AshtariEsfahani:2025ylh]
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[4-3]
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Real-time Signal Detection for Cyclotron Radiation Emission Spectroscopy Measurements using Antenna Arrays,
Ali Ashtari Esfahani et al.,
JINST 19 (2024) P05073,
arXiv:2310.02112.
[Project8:2023iju]
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[4-4]
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Cyclotron Radiation Emission Spectroscopy of Electrons from Tritium Beta Decay and $^{83\rm m}$Kr Internal Conversion,
A. Ashtari Esfahani et al.
(Project 8),
Phys.Rev.C 109 (2024) 035503,
arXiv:2303.12055.
[Project8:2023jkj]
-
[4-5]
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SYNCA: A Synthetic Cyclotron Antenna for the Project 8 Collaboration,
A. Ashtari Esfahani et al.,
JINST 18 (2023) P01034,
arXiv:2212.08026.
[Project8:2022kxg]
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[5-1]
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Going Big for Phase III of the Project 8 Neutrino Mass Experiment,
Juliana Stachurska
(Project 8),
PoS TAUP2023 (2024) 229,
arXiv:2311.16415.
TAUP 2023.
[Stachurska:2023ufl]
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[5-2]
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Project 8: R&D for a next-generation neutrino mass experiment,
Rene Reimann
(Project 8),
PoS PANIC2021 (2022) 283.
[Reimann:2022omy]
-
[5-3]
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Zero-deadtime processing in \beta spectroscopy for measurement of the non-zero neutrino mass,
Benjamin LaRoque
(Project 8),
EPJ Web Conf. 245 (2020) 01014.
[LaRoque:2020odr]
-
[5-4]
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Distributed Computing for the Project 8 Experiment,
Malachi Schram, Mathew Thomas, Kevin Fox, Benjamin LaRoque, Brent VanDevender, Noah Oblath, David Cowley
(Project 8),
EPJ Web Conf. 245 (2020) 03030.
[Schram:2020uqj]
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[5-5]
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Project 8: Towards a Direct Measurement of the Neutrino Mass with Tritium Beta Decays,
Noah Oblath
(Project 8),
PoS NEUTEL2017 (2018) 026.
[Oblath:2017xma]
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[5-6]
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Status of the Project 8 Phase II,
Mathieu Guigue
(Project 8),
J. Phys. Conf. Ser. 1342 (2020) 012025,
arXiv:1710.01827.
[Guigue:2017wzr]
-
[5-7]
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Overview of Project 8 and Progress Towards Tritium Operation,
Walter C. Pettus
(Project 8),
J. Phys. Conf. Ser. 1342 (2020) 012040,
arXiv:1710.01826.
[Pettus:2017sxd]
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[5-8]
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Direct neutrino mass measurement in the Project8 experiment,
Brent A. VanDevender
(PROJECT 8),
PoS HQL2016 (2017) 018.
[VanDevender:2016gnv]
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[5-9]
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Status of the neutrino mass experiments KATRIN and Project 8,
Florian Fraenkle,
PoS EPS-HEP2015 (2015) 084.
[Fraenkle:2015yfs]
-
[5-10]
-
Project 8: First Results & More,
Noah S. Oblath
(Project 8),
PoS NEUTEL2015 (2015) 046.
[Oblath:2015pxa]
-
[5-11]
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Project 8: Using Radio-Frequency Techniques to Measure Neutrino Mass,
N. S. Oblath
(Project 8),
arXiv:1310.0397, 2013.
Meeting of the APS Division of Particles and Fields.
[Oblath:2013rma]
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[5-12]
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Project 8: Determining neutrino mass from tritium $\beta$ decay using a frequency-based method,
P. J. Doe et al.
(Project 8),
arXiv:1309.7093, 2013.
Snowmass 2013}: {Snowmass on the Mississippi.
[Project8:2013trt]
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[5-14]
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Project 8: Update on a radiofrequency tritium spectrometer,
B. Monreal
(Project 8),
AIP Conf. Proc. 1441 (2012) 441-443.
[Monreal:2012zz]
Last Update: Thu 15 Oct 2026, 12:30:05 CET