HOLMES: The electron capture decay of 163Ho to measure the electron neutrino mass with sub-eV sensitivity
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G. Hilton | A. Giachero | S. Ragazzi | C. Reintsema | M. Sisti | G. Pessina | S. Nisi | A. Nucciotti | S. Heinitz | M. Biasotti | D. Corsini | F. Gatti | M. De Gerone | G. Pizzigoni | M. Balata | C. Brofferio | M. Faverzani | E. Ferri | M. Maino | F. Terranova | D. Bennett | J. Fowler | J. Hays-Wehle | D. Swetz | J. Ullom | R. Dressler | P. K. Day | V. Ceriale | D. Schumann | B. Alpert | G. Hilton | S. Ragazzi | U. Koester | P. Day | M. Biasotti | F. Gatti | C. Reintsema | J. Ullom | M. Maino | D. Schmidt | Andrea Giachero | M. Balata | S. Nisi | G. Pessina | F. Terranova | M. R. Gomes | R. Dressler | M. Sisti | J. Mates | J. Fowler | D. Swetz | S. Heinitz | D. Schumann | C. Boragno | D. Bennett | J. Hays-Wehle | A. Nucciotti | D. Corsini | C. Brofferio | V. Ceriale | M. Gerone | M. Faverzani | E. Ferri | M. Lusignoli | G. Pizzigoni | A. Puiu | B. Alpert | C. Boragno | U. Koester | M. Lusignoli | J. Mates | R. Nizzolo | A. Puiu | M. Ribeiro Gomes | D. Schmidt | R. Nizzolo
[1] Andrew S. Hoover,et al. Integration of TES Microcalorimeters With Microwave SQUID Multiplexed Readout , 2015, IEEE Transactions on Applied Superconductivity.
[2] L. Rosenberg,et al. Single-Electron Detection and Spectroscopy via Relativistic Cyclotron Radiation. , 2014, Physical review letters.
[3] R. Robertson. Can neutrino mass be measured in low-energy electron capture decay? , 2014 .
[4] Nathalie Palanque-Delabrouille,et al. Constraint on neutrino masses from SDSS-III/BOSS Lyα forest and other cosmological probes , 2014, 1410.7244.
[5] G. Kunde,et al. Integration of Radioactive Material with Microcalorimeter Detectors , 2014 .
[6] B. Dober,et al. MUSTANG2: a large focal plan array for the 100 meter Green Bank Telescope , 2014, Astronomical Telescopes and Instrumentation.
[7] A. Nucciotti. Statistical sensitivity of $$^{163}$$163Ho electron capture neutrino mass experiments , 2014, 1405.5060.
[8] D. Bagliani,et al. Thermal Properties of Holmium-Implanted Gold Films , 2014 .
[9] C. Kilbourne,et al. Preliminary Results of the MARE Experiment , 2014 .
[10] Joseph W. Fowler,et al. High-resolution gamma-ray spectroscopy with a microwave-multiplexed transition-edge sensor array , 2013, 1310.7287.
[11] F. M. Nortier,et al. Evaluation of 163Ho production options for neutrino mass measurements with microcalorimeter detectors , 2013 .
[12] B. Bumble,et al. ARCONS: A 2024 Pixel Optical through Near-IR Cryogenic Imaging Spectrophotometer , 2013, 1306.4674.
[13] K. Blaum,et al. The Electron Capture $$^{163}$$163Ho Experiment ECHo , 2013, 1309.5214.
[14] A. D. R'ujula. Two old ways to measure the electron-neutrino mass , 2013, 1305.4857.
[15] A. Singer,et al. Limit on sterile neutrino contribution from the Mainz Neutrino Mass Experiment , 2012, 1210.4194.
[16] Dan Werthimer,et al. A readout for large arrays of microwave kinetic inductance detectors. , 2012, The Review of scientific instruments.
[17] M. Günther,et al. 207 PRODUCTION OF RADIOISOTOPES WITH HIGH SPECIFIC ACTIVITY BY PHOTONUCLEAR REACTIONS: FROM A “WILD IDEA” TO REALITY , 2012 .
[18] S. Ragazzi,et al. The Electron Capture Decay of 163 Ho to Measure the Electron Neutrino Mass with sub-eV Accuracy and Beyond , 2012, 1202.4763.
[19] G. C. Hilton,et al. Code-division multiplexing for x-ray microcalorimeters , 2012, 1201.6289.
[20] N. M. Larson,et al. ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data , 2011 .
[21] M. Sorel,et al. The Search for neutrinoless double beta decay , 2011, 1109.5515.
[22] A. A. Golubev,et al. An upper limit on electron antineutrino mass from Troitsk experiment , 2011, 1108.5034.
[23] A. Letourneau,et al. The reactor antineutrino anomaly , 2011, 1101.2755.
[24] M. Vignati,et al. Relic antineutrino capture on 163Ho decaying nuclei , 2010, 1012.0760.
[25] Jonas Zmuidzinas,et al. Millimeter, Submillimeter, and Far-Infrared Detectors and Instrumentation for Astronomy V , 2016 .
[26] S. D. Rosner,et al. A Penning sputter ion source with very low energy spread , 2010 .
[27] M. Gonzalez-Garcia,et al. Updated global fit to three neutrino mixing: status of the hints of θ13 > 0 , 2010, 1001.4524.
[28] M. I. O. Technology,et al. Relativistic cyclotron radiation detection of tritium decay electrons as a new technique for measuring the neutrino mass , 2009, 0904.2860.
[29] E. Lisi,et al. Neutrino masses and mixing: 2008 status , 2009 .
[30] E. Otten,et al. Neutrino mass limit from tritium β decay , 2008, 0909.2104.
[31] D. Boyanovsky,et al. Constraints on dark matter particles from theory, galaxy observations and N-body simulations , 2007, 0710.5180.
[32] Christian Enss,et al. Cryogenic particle detection , 2005 .
[33] G. Hilton,et al. Transition-Edge Sensors , 2005 .
[34] B. Margesin,et al. New limits from the Milano neutrino mass experiment with thermal microcalorimeters , 2004 .
[35] B. Margesin,et al. Bolometric bounds on the antineutrino mass. , 2003, Physical review letters.
[36] Balraj Singh,et al. Nuclear Data Sheets for A = 163 , 2000 .
[37] Max Tegmark,et al. Weighing Neutrinos with Galaxy Surveys , 1997, astro-ph/9712057.
[38] A. Rújula,et al. Calorimetric measurements of 163holmium decay as tools to determine the electron neutrino mass , 1982 .
[39] Mau H. Chen,et al. Atomic electron excitation probabilities during orbital electron capture by the nucleus , 1979 .
[40] C. W. Nestor,et al. Calculation of Electron Shake-Off Probabilities as the Result of X-Ray Photoionization of the Rare Gases , 1973 .
[41] J. Power,et al. PREPARATION OF LONG-LIVED HOLMIUM-163 , 1960 .
[42] D. Shoenberg. Low Temperature Physics , 1948, Nature.
[43] E. Fermi. Versuch einer Theorie der β-Strahlen. I , 1934 .
[44] E. Fermi. An attempt of a theory of beta radiation. 1. , 1934 .