206 results on '"Gariazzo, S"'
Search Results
2. Non-standard cosmic expansion histories: Neutrino decoupling and primordial nucleosynthesis signatures
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Sierra, D. Aristizabal, Gariazzo, S., and Villanueva, A.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology - Abstract
Cosmological scenarios with a non-standard equation of state can involve ultrastiff fluids, understood as primordial fluids for which $p/\rho> 1$. Their energy densities can dominate the Universe energy budget at early times, in the otherwise radiation dominated epoch. During that period the Universe undergoes a faster expansion, that has implications for any decoupling process that takes place in that era. Quintessence models or Ekpyrotic cosmologies are good examples of such scenarios. Assuming the ultrastiff state to be thermally decoupled at very early times, if ever coupled, its observational imprints are left solely in the Universe expansion rate and in the radiation energy density. We consider a complete set of ultrastiff fluids and study their signatures in the neutrino decoupling and BBN eras. Measurements of $N_\text{eff}$ alone place mild constraints on these scenarios, with forthcoming measurements from the Simons Observatory in the Chilean Atacama desert being able to test regions where still sizable effects are observable. However, when BBN data is taken into account, those regions are proven to be barely reconcilable with primordial helium-4 and deuterium abundances measurements. Our findings show that measurements of the primordial helium-4 abundance imply the tightest constraints, with measurements of primordial deuterium being -- to a certain extent -- competitive as well. We point out that a $\sim 60\%$ improvement on the statistical uncertainty of the primordial helium-4 abundance measurement, will test these scenarios in the region where they can produce sizable effects. Beyond that precision the regions that are accessible degenerate with standard expectations. In that case, although potentially present, neither neutrino decoupling nor BBN observables will be sensitive probes., Comment: 13 pages, 7 figures, 2 tables. Matches publication in JCAP
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- 2023
3. Heisenberg's uncertainty principle in the PTOLEMY project: a theory update
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PTOLEMY Collaboration, Apponi, A., Betti, M. G., Borghesi, M., Boyarsky, A., Canci, N., Cavoto, G., Chang, C., Cheianov, V., Cheipesh, Y., Chung, W., Cocco, A. G., Colijn, A. P., D'Ambrosio, N., de Groot, N., Esposito, A., Faverzani, M., Ferella, A., Ferri, E., Ficcadenti, L., Frederico, T., Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Hochberg, Y., Kahn, Y., Lisanti, M., Mangano, G., Marcucci, L. E., Mariani, C., Marques, M., Menichetti, G., Messina, M., Mikulenko, O., Monticone, E., Nucciotti, A., Orlandi, D., Pandolfi, F., Parlati, S., Pepe, C., Heros, C. Pérez de los, Pisanti, O., Polini, M., Polosa, A. D., Puiu, A., Rago, I., Raitses, Y., Rajteri, M., Rossi, N., Rozwadowska, K., Rucandio, I., Ruocco, A., Strid, C. F., Tan, A., Teles, L. K., Tozzini, V., Tully, C. G., Viviani, M., Zeitler, U., and Zhao, F.
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High Energy Physics - Phenomenology ,Condensed Matter - Other Condensed Matter ,High Energy Physics - Experiment - Abstract
We discuss the consequences of the quantum uncertainty on the spectrum of the electron emitted by the $\beta$-processes of a tritium atom bound to a graphene sheet. We analyze quantitatively the issue recently raised in [Cheipesh et al., Phys. Rev. D 104, 116004 (2021)], and discuss the relevant time scales and the degrees of freedom that can contribute to the intrinsic spread in the electron energy. We perform careful calculations of the potential between tritium and graphene with different coverages and geometries. With this at hand, we propose possible avenues to mitigate the effect of the quantum uncertainty., Comment: 14 pages, 5 figures
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- 2022
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4. White Paper on Light Sterile Neutrino Searches and Related Phenomenology
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Acero, M. A., Argüelles, C. A., Hostert, M., Kalra, D., Karagiorgi, G., Kelly, K. J., Littlejohn, B., Machado, P., Pettus, W., Toups, M., Ross-Lonergan, M., Sousa, A., Surukuchi, P. T., Wong, Y. Y. Y., Abdallah, W., Abdullahi, A. M., Akutsu, R., Alvarez-Ruso, L., Alves, D. S. M., Aurisano, A., Balantekin, A. B., Berryman, J. M., Bertólez-Martínez, T., Brunner, J., Blennow, M., Bolognesi, S., Borusinski, M., Cianci, D., Collin, G., Conrad, J. M., Crow, B., Denton, P. B., Duvall, M., Fernández-Martinez, E., Fong, C. S., Foppiani, N., Forero, D. V., Friend, M., García-Soto, A., Giganti, C., Giunti, C., Gandhi, R., Ghosh, M., Hardin, J., Heeger, K. M., Ishitsuka, M., Izmaylov, A., Jones, B. J. P., Jordan, J. R., Kamp, N. W., Katori, T., Kim, S. B., Koerner, L. W., Lamoureux, M., Lasserre, T., Leach, K. G., Learned, J., Li, Y. F., Link, J. M., Louis, W. C., Mahn, K., Meyers, P. D., Maricic, J., Marko, D., Maruyama, T., Mertens, S., Minakata, H., Mocioiu, I., Mooney, M., Moulai, M. H., Nunokawa, H., Ochoa-Ricoux, J. P., Oh, Y. M., Ohlsson, T., Päs, H., Pershey, D., Robertson, R. G. H., Rosauro-Alcaraz, S., Rott, C., Roy, S., Salvado, J., Scott, M., Seo, S. H., Shaevitz, M. H., Smiley, M., Spitz, J., Stachurska, J., Thakore, T., Ternes, C. A., Thompson, A., Tseng, S., Vogelaar, B., Weiss, T., Wendell, R. A., Wright, T., Xin, Z., Yang, B. S., Yoo, J., Zennamo, J., Zettlemoyer, J., Zornoza, J. D., Ahmad, S., Basto-Gonzalez, V. S., Bowden, N. S., Cañas, B. C., Caratelli, D., Chang, C. V., Chen, C., Classen, T., Convery, M., Davies, G. S., Dennis, S. R., Djurcic, Z., Dorrill, R., Du, Y., Evans, J. J., Fahrendholz, U., Formaggio, J. A., Foust, B. T., Gatti, H. Frandini, Garcia-Gamez, D., Gariazzo, S., Gehrlein, J., Grant, C., Gomes, R. A., Hansell, A. B., Halzen, F., Ho, S., Zink, J. Hoefken, Jones, R. S., Kunkle, P., Li, J. -Y., Li, S. C., Luo, X., Malyshkin, Yu., Massaro, D., Mastbaum, A., Mohanta, R., Mumm, H. P., Nebot-Guinot, M., Neilson, R., Ni, K., Nieves, J., Gann, G. D. Orebi, Pandey, V., Pascoli, S., Qian, X., Rajaoalisoa, M., Roca, C., Roskovec, B., Saul-Sala, E., Saldaña, L., Scholberg, K., Shakya, B., Slocum, P. L., Snider, E. L., Steiger, H. Th. J., Steklain, A. F., Stock, M. R., Sutanto, F., Takhistov, V., Tsai, Y. -D., Tsai, Y. -T., Venegas-Vargas, D., Wallbank, M., Wang, E., Weatherly, P., Westerdale, S., Worcester, E., Wu, W., Yang, G., and Zamorano, B.
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High Energy Physics - Experiment ,Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology ,Physics - Instrumentation and Detectors - Abstract
This white paper provides a comprehensive review of our present understanding of experimental neutrino anomalies that remain unresolved, charting the progress achieved over the last decade at the experimental and phenomenological level, and sets the stage for future programmatic prospects in addressing those anomalies. It is purposed to serve as a guiding and motivational "encyclopedic" reference, with emphasis on needs and options for future exploration that may lead to the ultimate resolution of the anomalies. We see the main experimental, analysis, and theory-driven thrusts that will be essential to achieving this goal being: 1) Cover all anomaly sectors -- given the unresolved nature of all four canonical anomalies, it is imperative to support all pillars of a diverse experimental portfolio, source, reactor, decay-at-rest, decay-in-flight, and other methods/sources, to provide complementary probes of and increased precision for new physics explanations; 2) Pursue diverse signatures -- it is imperative that experiments make design and analysis choices that maximize sensitivity to as broad an array of these potential new physics signatures as possible; 3) Deepen theoretical engagement -- priority in the theory community should be placed on development of standard and beyond standard models relevant to all four short-baseline anomalies and the development of tools for efficient tests of these models with existing and future experimental datasets; 4) Openly share data -- Fluid communication between the experimental and theory communities will be required, which implies that both experimental data releases and theoretical calculations should be publicly available; and 5) Apply robust analysis techniques -- Appropriate statistical treatment is crucial to assess the compatibility of data sets within the context of any given model., Comment: Contribution to Snowmass 2021 by the NF02 Topical Group (Understanding Experimental Neutrino Anomalies). Published in J. Phys. G as a Major Report
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- 2022
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5. Implementation and Optimization of the PTOLEMY Transverse Drift Electromagnetic Filter
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Apponi, A., Betti, M. G., Borghesi, M., Boscá, A., Calle, F., Canci, N., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., D'Ambrosio, N., de Groot, N., Faverzani, M., Ferella, A., Ferri, E., Ficcadenti, L., Garcia-Abia, P., Gomez-Tejedor, G. Garcia, Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Hochberg, Y., Kahn, Y., Kievsky, A., Lisanti, M., Mangano, G., Marcucci, L. E., Mariani, C., Martínez, J., Messina, M., Monticone, E., Nucciotti, A., Orlandi, D., Pandolfi, F., Parlati, S., Pedrós, J., Heros, C. Pérez de los, Pisanti, O., Polosa, A. D., Puiu, A., Rago, I., Raitses, Y., Rajteri, M., Rossi, N., Rozwadowska, K., Rucandio, I., Ruocco, A., Santorelli, R., Strid, C. F., Tan, A., Tully, C. G., Viviani, M., Zeitler, U., and Zhao, F.
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Physics - Instrumentation and Detectors ,Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
The PTOLEMY transverse drift filter is a new concept to enable precision analysis of the energy spectrum of electrons near the tritium beta-decay endpoint. This paper details the implementation and optimization methods for successful operation of the filter. We present the first demonstrator that produces the required magnetic field properties with an iron return-flux magnet. Two methods for the setting of filter electrode voltages are detailed. The challenges of low-energy electron transport in cases of low field are discussed, such as the growth of the cyclotron radius with decreasing magnetic field, which puts a ceiling on filter performance relative to fixed filter dimensions. Additionally, low pitch angle trajectories are dominated by motion parallel to the magnetic field lines and introduce non-adiabatic conditions and curvature drift. To minimize these effects and maximize electron acceptance into the filter, we present a three-potential-well design to simultaneously drain the parallel and transverse kinetic energies throughout the length of the filter. These optimizations are shown, in simulation, to achieve low-energy electron transport from a 1 T iron core (or 3 T superconducting) starting field with initial kinetic energy of 18.6 keV drained to <10 eV (<1 eV) in about 80 cm. This result for low field operation paves the way for the first demonstrator of the PTOLEMY spectrometer for measurement of electrons near the tritium endpoint to be constructed at the Gran Sasso National Laboratary (LNGS) in Italy., Comment: 29 pages, 25 figures
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- 2021
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6. PArthENoPE Revolutions
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Gariazzo, S., de Salas, P. F., Pisanti, O., and Consiglio, R.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
This paper presents the main features of a new and updated version of the program PArthENoPE, which the community has been using for many years for computing the abundances of light elements produced during Big Bang Nucleosynthesis. This is the third release of the PArthENoPE code, after the 2008 and the 2018 ones, and will be distributed from the code's website, http://parthenope.na.infn.it. Apart from minor changes, the main improvements in this new version include a revisited implementation of the nuclear rates for the most important reactions of deuterium destruction, H2(p,gamma)He3, H2(d, n)He3 and H2(d, p)H3, and a re-designed GUI, which extends the functionality of the previous one. The new GUI, in particular, supersedes the previous tools for running over grids of parameters with a better management of parallel runs, and it offers a brand-new set of functions for plotting the results., Comment: 28 pages, 7 figures
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- 2021
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7. 2020 Global reassessment of the neutrino oscillation picture
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de Salas, P. F., Forero, D. V., Gariazzo, S., Martínez-Miravé, P., Mena, O., Ternes, C. A., Tórtola, M., and Valle, J. W. F.
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High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment - Abstract
We present an updated global fit of neutrino oscillation data in the simplest three-neutrino framework. In the present study we include up-to-date analyses from a number of experiments. Concerning the atmospheric and solar sectors, we give updated analyses of DeepCore and SNO data, respectively. We have also included the latest electron antineutrino data collected by the Daya Bay and RENO reactor experiments, and the long-baseline T2K and NO$\nu$A measurements. These new analyses result in more accurate measurements of $\theta_{13}$, $\theta_{12}$, $\Delta m_{21}^2$ and $|\Delta m_{31}^2|$. The best fit value for the atmospheric angle $\theta_{23}$ lies in the second octant, but first octant solutions remain allowed at $\sim2.4\sigma$. Regarding CP violation measurements, the preferred value of $\delta$ we obtain is 1.08$\pi$ (1.58$\pi$) for normal (inverted) neutrino mass ordering. The global analysis prefers normal neutrino mass ordering with 2.5$\sigma$. This preference is milder than the one found in previous global analyses. The new results should be regarded as robust due to the agreement found between our Bayesian and frequentist approaches. Taking into account only oscillation data, there is a weak/moderate preference for the normal neutrino mass ordering of $2.00\sigma$. While adding neutrinoless double beta decay from the latest Gerda, CUORE and KamLAND-Zen results barely modifies this picture, cosmological measurements raise the preference to $2.68\sigma$ within a conservative approach. A more aggressive data set combination of cosmological observations leads to a similar preference, namely $2.70\sigma$. This very same cosmological data set provides $2\sigma$ upper limits on the total neutrino mass corresponding to $\sum\nu<0.12$ ($0.15$)~eV for normal (inverted) neutrino mass ordering., Comment: 35 pages, 15 figures, 3 tables, version 2 includes updated analyses of reactor and accelerator data, matches version accepted for publication in JHEP
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- 2020
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8. Light sterile neutrinos: the current picture from neutrino oscillations
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Gariazzo, S.
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High Energy Physics - Phenomenology - Abstract
Light sterile neutrinos with a mass around 1 eV have been studied for many years as a possible explanation of the so called short-baseline neutrino oscillation anomalies. Recently, several neutrino oscillation experiments reported preferences for non-zero values of the mixing angles and squared mass differences for active-sterile mixing, which however are not always in agreement. I will review our current knowledge on the light sterile neutrino in the 3+1 model, starting with a separate discussion on the status of the most relevant searches and then analyzing the problems that arise when combining different probes in a global fit., Comment: To appear in the Proceedings of TAUP 2019, Toyama, Japan, September 9-13, 2019. arXiv admin note: substantial text overlap with arXiv:1910.13172
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- 2019
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9. Relic neutrinos: local clustering and consequences for direct detection
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Gariazzo, S.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology - Abstract
The Cosmic Neutrino Background is a prediction of the standard cosmological model, but it has been never observed directly. Experiments with the aim of detecting relic CNB neutrinos are under development. For such experiments, the expected event rate depends on the local number density of relic neutrinos. Since massive neutrinos can be attracted by the gravitational potential of our galaxy and cluster locally, a local overdensity of relic neutrinos should exist at Earth. We report the status of our knowledge on the clustering of neutrinos and the consequences for future direct detection experiments., Comment: To appear in the Proceedings of the European Physical Society Conference on High Energy Physics (EPS-HEP 2019), Ghent, Belgium, 10-17 July, 2019
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- 2019
10. Light sterile neutrinos: oscillations and cosmology
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Gariazzo, S.
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High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Light sterile neutrinos with a mass around 1 eV have been studied for many years as a possible explanation of the so called short-baseline neutrino oscillation anomalies. Recently, several neutrino oscillation experiments reported preferences for non-zero values of the mixing angles and squared mass differences for active-sterile mixing, which however are not always in agreement. I review our current knowledge of the light sterile neutrino in the 3+1 model, starting with a separate discussion on the status of the most relevant searches and then analyzing the problems that arise when combining different probes in a global fit. A short summary on the tension with cosmological observations is also provided., Comment: To appear in the Proceedings of "Matter To The Deepest", XLIII International Conference of Theoretical Physics, Katowice/Chorz\'ow, Poland, 1-6 September 2019
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- 2019
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11. Neutrino clustering in the Milky Way and beyond
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Mertsch, P., Parimbelli, G., de Salas, P. F., Gariazzo, S., Lesgourgues, J., and Pastor, S.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology - Abstract
The standard cosmological model predicts the existence of a Cosmic Neutrino Background, which has not yet been observed directly. Some experiments aiming at its detection are currently under development, despite the tiny kinetic energy of the cosmological relic neutrinos, which makes this task incredibly challenging. Since massive neutrinos are attracted by the gravitational potential of our Galaxy, they can cluster locally. Neutrinos should be more abundant at the Earth position than at an average point in the Universe. This fact may enhance the expected event rate in any future experiment. Past calculations of the local neutrino clustering factor only considered a spherical distribution of matter in the Milky Way and neglected the influence of other nearby objects like the Virgo cluster, although recent $N$-body simulations suggest that the latter may actually be important. In this paper, we adopt a back-tracking technique, well established in the calculation of cosmic rays fluxes, to perform the first three-dimensional calculation of the number density of relic neutrinos at the Solar System, taking into account not only the matter composition of the Milky Way, but also the contribution of the Andromeda galaxy and the Virgo cluster. The effect of Virgo is indeed found to be relevant and to depend non-trivially on the value of the neutrino mass. Our results show that the local neutrino density is enhanced by 0.53% for a neutrino mass of 10 meV, 12% for 50 meV, 50% for 100 meV or 500% for 300 meV., Comment: 24 pages, 5 figures
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- 2019
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12. Proceedings of The Magnificent CE$\nu$NS Workshop 2018
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Sierra, D. Aristizabal, Balantekin, A. B., Caratelli, D., Cogswell, B., Collar, J. I., Dahl, C. E., Dent, J., Dutta, B., Engel, J., Estrada, J., Formaggio, J., Gariazzo, S., Han, R., Hedges, S., Huber, P., Konovalov, A., Lang, R. F., Liao, S., Lindner, M., Machado, P., Mahapatra, R., Marfatia, D., Martinez-Soler, I., Miranda, O., Misiak, D., Naumov, D. V., Newby, J., Newstead, J., Papoulias, D., Patton, K., Pereverzev, S., Pospelov, M., Scholberg, K., Sinev, G., Strauss, R., Strigari, L., Tayloe, R., Tiffenberg, J., Vidal, M., Vignati, M., Wagner, V., Walker, J., Yu, T. -T., Zettlemoyer, J., and Rich, G. C.
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High Energy Physics - Experiment ,Astrophysics - Instrumentation and Methods for Astrophysics ,High Energy Physics - Phenomenology ,Nuclear Experiment ,Physics - Instrumentation and Detectors - Abstract
The Magnificent CE$\nu$NS Workshop (2018) was held November 2 & 3 of 2018 on the University of Chicago campus and brought together theorists, phenomenologists, and experimentalists working in numerous areas but sharing a common interest in the process of coherent elastic neutrino-nucleus scattering (CE$\nu$NS). This is a collection of abstract-like summaries of the talks given at the meeting, including links to the slides presented. This document and the slides from the meeting provide an overview of the field and a snapshot of the robust CE$\nu$NS-related efforts both planned and underway., Comment: The Magnificent CEvNS Workshop (2018), Nov 2-3, 2018; Chicago, IL, USA; 44 contributions
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- 2019
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13. Constraining power of open likelihoods, made prior-independent
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Gariazzo, S.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology ,Physics - Data Analysis, Statistics and Probability - Abstract
One of the most criticized features of Bayesian statistics is the fact that credible intervals, especially when open likelihoods are involved, may strongly depend on the prior shape and range. Many analyses involving open likelihoods are affected by the eternal dilemma of choosing between linear and logarithmic prior, and in particular in the latter case the situation is worsened by the dependence on the prior range under consideration. In this letter, we revive a simple method to obtain constraints that depend neither on the prior shape nor range and, using the tools of Bayesian model comparison, extend it to overcome the possible dependence of the bounds on the choice of free parameters in the numerical analysis. An application to the case of cosmological bounds on the sum of the neutrino masses is discussed as an example., Comment: 6 pages, 3 figures; matches version accepted for publication in EPJC
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- 2019
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14. Thermalisation of sterile neutrinos in the early Universe in the 3+1 scheme with full mixing matrix
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Gariazzo, S., de Salas, P. F., and Pastor, S.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology - Abstract
In the framework of a 3+1 scheme with an additional inert state, we consider the thermalisation of sterile neutrinos in the early Universe taking into account the full $4\times4$ mixing matrix. The evolution of the neutrino energy distributions is found solving the momentum-dependent kinetic equations with full diagonal collision terms, as in previous analyses of flavour neutrino decoupling in the standard case. The degree of thermalisation of the sterile state is shown in terms of the effective number of neutrinos, $N_{\rm eff}$, and its dependence on the three additional mixing angles ($\theta_{14}$, $\theta_{24}$, $\theta_{34}$) and on the squared mass difference $\Delta m^2_{41}$ is discussed. Our results are relevant for fixing the contribution of a fourth light neutrino species to the cosmological energy density, whose value is very well constrained by the final Planck analysis. For the preferred region of active-sterile mixing parameters from short-baseline neutrino experiments, we find that the fourth state is fully thermalised ($N_{\rm eff}\simeq 4$)., Comment: 30 pages, 10 figures. Matches published version
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- 2019
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15. Neutrino physics with the PTOLEMY project: active neutrino properties and the light sterile case
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PTOLEMY collaboration, Betti, M. G., Biasotti, M., Boscá, A., Calle, F., Cavoto, G., Chang, C., Cocco, A. G., Colijn, A. P., Conrad, J., D'Ambrosio, N., De Groot, N., de Salas, P. F., Faverzani, M., Ferella, A., Ferri, E., Garcia-Abia, P., García-Cortés, I., Gomez-Tejedor, G. Garcia, Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Gudmundsson, J. E., Hochberg, Y., Kahn, Y., Kievsky, A., Lisanti, M., Mancini-Terracciano, C., Mangano, G., Marcucci, L. E., Mariani, C., Martínez, J., Messina, M., Molinero-Vela, A., Monticone, E., Moroño, A., Nucciotti, A., Pandolfi, F., Parlati, S., Pastor, S., Pedrós, J., Heros, C. Pérez de los, Pisanti, O., Polosa, A. D., Puiu, A., Rago, I., Raitses, Y., Rajteri, M., Rossi, N., Rucandio, I., Santorelli, R., Schaeffner, K., Tully, C. G., Viviani, M., Zhao, F., and Zurek, K. M.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment ,High Energy Physics - Phenomenology - Abstract
The PTOLEMY project aims to develop a scalable design for a Cosmic Neutrino Background (CNB) detector, the first of its kind and the only one conceived that can look directly at the image of the Universe encoded in neutrino background produced in the first second after the Big Bang. The scope of the work for the next three years is to complete the conceptual design of this detector and to validate with direct measurements that the non-neutrino backgrounds are below the expected cosmological signal. In this paper we discuss in details the theoretical aspects of the experiment and its physics goals. In particular, we mainly address three issues. First we discuss the sensitivity of PTOLEMY to the standard neutrino mass scale. We then study the perspectives of the experiment to detect the CNB via neutrino capture on tritium as a function of the neutrino mass scale and the energy resolution of the apparatus. Finally, we consider an extra sterile neutrino with mass in the eV range, coupled to the active states via oscillations, which has been advocated in view of neutrino oscillation anomalies. This extra state would contribute to the tritium decay spectrum, and its properties, mass and mixing angle, could be studied by analyzing the features in the beta decay electron spectrum., Comment: Typos corrected; Matches version accepted by JCAP
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- 2019
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16. Cosmology-marginalized approaches in Bayesian model comparison: the neutrino mass as a case study
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Gariazzo, S. and Mena, O.
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Astrophysics - Cosmology and Nongalactic Astrophysics ,Astrophysics - Instrumentation and Methods for Astrophysics ,High Energy Physics - Phenomenology ,Physics - Data Analysis, Statistics and Probability - Abstract
We propose here a \emph{novel} method which singles out the \emph{a priori} unavoidable dependence on the underlying cosmological model when extracting parameter constraints, providing robust limits which only depend on the considered dataset. Interestingly, when dealing with several possible cosmologies and interpreting the Bayesian preference in terms of the Gaussian statistical evidence, the preferred model is much less favored than when only two cases are compared. As a working example, we apply our approach to the cosmological neutrino mass bounds, which play a fundamental role not only in establishing the contribution of relic neutrinos to the dark matter of the Universe, but also in the planning of future experimental searches of the neutrino character and of the neutrino mass ordering., Comment: 6 pages, 1 table, 2 figures; matches version accepted for publication in PRD
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- 2018
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17. A Design for an Electromagnetic Filter for Precision Energy Measurements at the Tritium Endpoint
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Betti, M. G., Biasotti, M., Bosca, A., Calle, F., Carabe-Lopez, J., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., Conrad, J., D'Ambrosio, N., de Salas, P. F., Faverzani, M., Ferella, A., Ferri, E., Garcia-Abia, P., Gomez-Tejedor, G. Garcia, Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Gudmundsson, J., Hochberg, Y., Kahn, Y., Lisanti, M., Mancini-Terracciano, C., Mangano, G., Marcucci, L. E., Mariani, C., Martinez, J., Messina, M., Molinero-Vela, A., Monticone, E., Nucciotti, A., Pandolfi, F., Pastor, S., Pedros, J., Heros, C. Perez de los, Pisanti, O., Polosa, A., Puiu, A., Raitses, Y., Rajteri, M., Rossi, N., Santorelli, R., Schaeffner, K., Strid, C. F., Tully, C. G., Zhao, F., and Zurek, K. M.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Physics - Instrumentation and Detectors - Abstract
We present a detailed description of the electromagnetic filter for the PTOLEMY project to directly detect the Cosmic Neutrino Background (CNB). Starting with an initial estimate for the orbital magnetic moment, the higher-order drift process of ExB is configured to balance the gradient-B drift motion of the electron in such a way as to guide the trajectory into the standing voltage potential along the mid-plane of the filter. As a function of drift distance along the length of the filter, the filter zooms in with exponentially increasing precision on the transverse velocity component of the electron kinetic energy. This yields a linear dimension for the total filter length that is exceptionally compact compared to previous techniques for electromagnetic filtering. The parallel velocity component of the electron kinetic energy oscillates in an electrostatic harmonic trap as the electron drifts along the length of the filter. An analysis of the phase-space volume conservation validates the expected behavior of the filter from the adiabatic invariance of the orbital magnetic moment and energy conservation following Liouville's theorem for Hamiltonian systems.
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- 2018
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18. PTOLEMY: A Proposal for Thermal Relic Detection of Massive Neutrinos and Directional Detection of MeV Dark Matter
- Author
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Baracchini, E., Betti, M. G., Biasotti, M., Bosca, A., Calle, F., Carabe-Lopez, J., Cavoto, G., Chang, C., Cocco, A. G., Colijn, A. P., Conrad, J., D'Ambrosio, N., de Salas, P. F., Faverzani, M., Ferella, A., Ferri, E., Garcia-Abia, P., Gomez-Tejedor, G. Garcia, Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Gudmundsson, J., Hochberg, Y., Kahn, Y., Lisanti, M., Mancini-Terracciano, C., Mangano, G., Marcucci, L. E., Mariani, C., Martinez, J., Mazzitelli, G., Messina, M., Molinero-Vela, A., Monticone, E., Nucciotti, A., Pandolfi, F., Pastor, S., Pedros, J., Heros, C. Perez de los, Pisanti, O., Polosa, A., Puiu, A., Rajteri, M., Santorelli, R., Schaeffner, K., Tully, C. G., Raitses, Y., Rossi, N., Zhao, F., and Zurek, K. M.
- Subjects
Physics - Instrumentation and Detectors ,Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment - Abstract
We propose to achieve the proof-of-principle of the PTOLEMY project to directly detect the Cosmic Neutrino Background (CNB). Each of the technological challenges described in [1,2] will be targeted and hopefully solved by the use of the latest experimental developments and profiting from the low background environment provided by the LNGS underground site. The first phase will focus on the graphene technology for a tritium target and the demonstration of TES microcalorimetry with an energy resolution of better than 0.05 eV for low energy electrons. These technologies will be evaluated using the PTOLEMY prototype, proposed for underground installation, using precision HV controls to step down the kinematic energy of endpoint electrons to match the calorimeter dynamic range and rate capabilities. The second phase will produce a novel implementation of the EM filter that is scalable to the full target size and which demonstrates intrinsic triggering capability for selecting endpoint electrons. Concurrent with the CNB program, we plan to exploit and develop the unique properties of graphene to implement an intermediate program for direct directional detection of MeV dark matter [3,4]. This program will evaluate the radio-purity and scalability of the graphene fabrication process with the goal of using recently identified ultra-high radio-purity CO2 sources. The direct detection of the CNB is a snapshot of early universe dynamics recorded by the thermal relic neutrino yield taken at a time that predates the epochs of Big Bang Nucleosynthesis, the Cosmic Microwave Background and the recession of galaxies (Hubble Expansion). Big Bang neutrinos are believed to have a central role in the evolution of the Universe and a direct measurement with PTOLEMY will unequivocally establish the extent to which these predictions match present-day neutrino densities.
- Published
- 2018
19. Neutrino mass eigenstates and their ordering: a Bayesian approach
- Author
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Gariazzo, S.
- Subjects
High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
One of the not-yet determined properties of neutrinos is the ordering of their mass eigenstates. We combine the available data from neutrino oscillations, neutrinoless double beta decay and Cosmic Microwave Background observations to derive robust constraints on the mass ordering in a Bayesian context. Based on arxiv:1801.04946., Comment: 3 pages, 2 figures. To appear in the Proceedings of Incontri di Fisica delle Alte Energie (IFAE) 2018
- Published
- 2018
20. Neutrino Mass Ordering from Oscillations and Beyond: 2018 Status and Future Prospects
- Author
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de Salas, P. F., Gariazzo, S., Mena, O., Ternes, C. A., and Tórtola, M.
- Subjects
High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
The ordering of the neutrino masses is a crucial input for a deep understanding of flavor physics, and its determination may provide the key to establish the relationship among the lepton masses and mixings and their analogous properties in the quark sector. The extraction of the neutrino mass ordering is a data-driven field expected to evolve very rapidly in the next decade. In this review, we both analyze the present status and describe the physics of subsequent prospects. Firstly, the different current available tools to measure the neutrino mass ordering are described. Namely, reactor, long-baseline (accelerator and atmospheric) neutrino beams, laboratory searches for beta and neutrinoless double beta decays and observations of the cosmic background radiation and the large scale structure of the universe are carefully reviewed. Secondly, the results from an up-to-date comprehensive global fit are reported: the Bayesian analysis to the 2018 publicly available oscillation and cosmological data sets provides \emph{strong} evidence for the normal neutrino mass ordering versus the inverted scenario, with a significance of 3.5 standard deviations. This preference for the normal neutrino mass ordering is mostly due to neutrino oscillation measurements. Finally, we shall also emphasize the future perspectives for unveiling the neutrino mass ordering. In this regard, apart from describing the expectations from the aforementioned probes, we also focus on those arising from alternative and novel methods, as 21~cm cosmology, core-collapse supernova neutrinos and the direct detection of relic neutrinos., Comment: 62 pages, 3 Tables and 15 figures. Invited Review for the 'Frontiers in Astronomy and Space Science' - Section 'High Energy and Astroparticle Physics', Research Topic 'From the Fermi Scale to Cosmology'. v2 matches the version accepted for publication
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- 2018
- Full Text
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21. PTOLEMY: Relic neutrino direct detection
- Author
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Mead, J, Apponi, A, Betti, M, Borghesi, M, Castellano, O, Cavoto, G, Celasco, E, Chung, W, Cocco, A, Colijn, A, Cortis, D, D'Ambrosio, N, de Groot, N, el Morabit, S, Esposito, A, Farino, M, Faverzani, M, Ferri, E, Ficcadenti, L, Gariazzo, S, Garrone, H, Gatti, F, Giachero, A, Iwasaki, Y, Laubenstein, M, Manenti, L, Mangano, G, Marcucci, L, Mariani, C, Menichetti, G, Messina, M, Monticone, E, Naafs, M, Nucciotti, A, Pandolfi, F, Paoloni, D, Pepe, C, Pérez de los Heros, C, Pisanti, O, Pofi, F, Polosa, A, Puiu, A, Rago, I, Rajteri, M, Rossi, N, Ruocco, A, Tan, A, Tozzini, V, Tully, C, van Rens, I, Virzi, F, Visser, G, Viviani, M, Zeitler, U, Zheliuk, O, Zimmer, F, Mead J. V., Apponi A., Betti M., Borghesi M., Castellano O., Cavoto G., Celasco E., Chung W., Cocco A., Colijn A., Cortis D., D'Ambrosio N., de Groot N., el Morabit S., Esposito A., Farino M., Faverzani M., Ferri E., Ficcadenti L., Gariazzo S., Garrone H., Gatti F., Giachero A., Iwasaki Y., Laubenstein M., Manenti L., Mangano G., Marcucci L. E., Mariani C., Mead J., Menichetti G., Messina M., Monticone E., Naafs M., Nucciotti A., Pandolfi F., Paoloni D., Pepe C., Pérez de los Heros C., Pisanti O., Pofi F. M., Polosa A. D., Puiu A., Rago I., Rajteri M., Rossi N., Ruocco A., Tan A., Tozzini V., Tully C., van Rens I., Virzi F., Visser G., Viviani M., Zeitler U., Zheliuk O., Zimmer F., Mead, J, Apponi, A, Betti, M, Borghesi, M, Castellano, O, Cavoto, G, Celasco, E, Chung, W, Cocco, A, Colijn, A, Cortis, D, D'Ambrosio, N, de Groot, N, el Morabit, S, Esposito, A, Farino, M, Faverzani, M, Ferri, E, Ficcadenti, L, Gariazzo, S, Garrone, H, Gatti, F, Giachero, A, Iwasaki, Y, Laubenstein, M, Manenti, L, Mangano, G, Marcucci, L, Mariani, C, Menichetti, G, Messina, M, Monticone, E, Naafs, M, Nucciotti, A, Pandolfi, F, Paoloni, D, Pepe, C, Pérez de los Heros, C, Pisanti, O, Pofi, F, Polosa, A, Puiu, A, Rago, I, Rajteri, M, Rossi, N, Ruocco, A, Tan, A, Tozzini, V, Tully, C, van Rens, I, Virzi, F, Visser, G, Viviani, M, Zeitler, U, Zheliuk, O, Zimmer, F, Mead J. V., Apponi A., Betti M., Borghesi M., Castellano O., Cavoto G., Celasco E., Chung W., Cocco A., Colijn A., Cortis D., D'Ambrosio N., de Groot N., el Morabit S., Esposito A., Farino M., Faverzani M., Ferri E., Ficcadenti L., Gariazzo S., Garrone H., Gatti F., Giachero A., Iwasaki Y., Laubenstein M., Manenti L., Mangano G., Marcucci L. E., Mariani C., Mead J., Menichetti G., Messina M., Monticone E., Naafs M., Nucciotti A., Pandolfi F., Paoloni D., Pepe C., Pérez de los Heros C., Pisanti O., Pofi F. M., Polosa A. D., Puiu A., Rago I., Rajteri M., Rossi N., Ruocco A., Tan A., Tozzini V., Tully C., van Rens I., Virzi F., Visser G., Viviani M., Zeitler U., Zheliuk O., and Zimmer F.
- Published
- 2024
22. Cosmic Neutrino Background detection with PTOLEMY
- Author
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Rossi, N, Apponi, A, Betti, M, Borghesi, M, Castellano, O, Cavoto, G, Celasco, E, Chung, W, Cocco, A, Colijn, A, Cortis, D, D'Ambrosio, N, de Groot, N, el Morabit, S, Esposito, A, Farino, M, Faverzani, M, Ferri, E, Ficcadenti, L, Gariazzo, S, Garrone, H, Gatti, F, Giachero, A, Iwasaki, Y, Laubenstein, M, Manenti, L, Mangano, G, Marcucci, L, Mariani, C, Mead, J, Menichetti, G, Messina, M, Monticone, E, Naafs, M, Nucciotti, A, Pandolfi, F, Paoloni, D, Pepe, C, de los Heros, C, Pisanti, O, Pofi, F, Polosa, A, Puiu, A, Rago, I, Rajteri, M, Ruocco, A, Tan, A, Tozzini, V, Tully, C, van Rens, I, Virzi, F, Visser, G, Viviani, M, Zeitler, U, Zheliuk, O, Zimmer, F, Rossi N., Apponi A., Betti M. G., Borghesi M., Castellano O., Cavoto G., Celasco E., Chung W., Cocco A., Colijn A., Cortis D., D'Ambrosio N., de Groot N., el Morabit S., Esposito A., Farino M., Faverzani M., Ferri E., Ficcadenti L., Gariazzo S., Garrone H., Gatti F., Giachero A., Iwasaki Y., Laubenstein M., Manenti L., Mangano G., Marcucci L. E., Mariani C., Mead J., Menichetti G., Messina M., Monticone E., Naafs M., Nucciotti A., Pandolfi F., Paoloni D., Pepe C., de los Heros C. P., Pisanti O., Pofi F., Polosa A. D., Puiu A., Rago I., Rajteri M., Ruocco A., Tan A., Tozzini V., Tully C., van Rens I., Virzi F., Visser G., Viviani M., Zeitler U., Zheliuk O., Zimmer F., Rossi, N, Apponi, A, Betti, M, Borghesi, M, Castellano, O, Cavoto, G, Celasco, E, Chung, W, Cocco, A, Colijn, A, Cortis, D, D'Ambrosio, N, de Groot, N, el Morabit, S, Esposito, A, Farino, M, Faverzani, M, Ferri, E, Ficcadenti, L, Gariazzo, S, Garrone, H, Gatti, F, Giachero, A, Iwasaki, Y, Laubenstein, M, Manenti, L, Mangano, G, Marcucci, L, Mariani, C, Mead, J, Menichetti, G, Messina, M, Monticone, E, Naafs, M, Nucciotti, A, Pandolfi, F, Paoloni, D, Pepe, C, de los Heros, C, Pisanti, O, Pofi, F, Polosa, A, Puiu, A, Rago, I, Rajteri, M, Ruocco, A, Tan, A, Tozzini, V, Tully, C, van Rens, I, Virzi, F, Visser, G, Viviani, M, Zeitler, U, Zheliuk, O, Zimmer, F, Rossi N., Apponi A., Betti M. G., Borghesi M., Castellano O., Cavoto G., Celasco E., Chung W., Cocco A., Colijn A., Cortis D., D'Ambrosio N., de Groot N., el Morabit S., Esposito A., Farino M., Faverzani M., Ferri E., Ficcadenti L., Gariazzo S., Garrone H., Gatti F., Giachero A., Iwasaki Y., Laubenstein M., Manenti L., Mangano G., Marcucci L. E., Mariani C., Mead J., Menichetti G., Messina M., Monticone E., Naafs M., Nucciotti A., Pandolfi F., Paoloni D., Pepe C., de los Heros C. P., Pisanti O., Pofi F., Polosa A. D., Puiu A., Rago I., Rajteri M., Ruocco A., Tan A., Tozzini V., Tully C., van Rens I., Virzi F., Visser G., Viviani M., Zeitler U., Zheliuk O., and Zimmer F.
- Abstract
The PTOLEMY experiment aims at detecting the cosmic neutrino background, generated approximately one second after the Big Bang, in accordance with Standard Cosmology. Given the extremely low energy of these neutrinos, reliable experimental detection can be accomplished through neutrino captures on beta-unstable nuclides, eliminating the need for a specific energy threshold. Tritium implanted on a carbon-based nanostructure emerges as a promising candidate among the various isotopes due to its favorable cross-section and low-endpoint energy. The Ptolemy collaboration plans to integrate a solid-state tritium source with a novel compact electromagnetic filter, based on the dynamic transverse momentum cancellation concept. This filter will be employed in conjunction with an event-based preliminary radio-frequency preselection. The measurement of neutrino mass and the exploration of light sterile neutrinos represent additional outcomes stemming from the Ptolemy experiment’s physics potential, even when utilizing smaller or intermediate-scale detectors. To finalize the conceptualization of the detector, a demonstrator prototype will be assembled and tested at LNGS in 2024. This prototype aims at addressing the challenging aspects of the Ptolemy experiment.
- Published
- 2024
23. Cosmological bounds on neutrino statistics
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de Salas, P. F., Gariazzo, S., Laveder, M., Pastor, S., Pisanti, O., and Truong, N.
- Subjects
Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Phenomenology - Abstract
We consider the phenomenological implications of the violation of the Pauli exclusion principle for neutrinos, focusing on cosmological observables such as the spectrum of Cosmic Microwave Background anisotropies, Baryon Acoustic Oscillations and the primordial abundances of light elements. Neutrinos that behave (at least partly) as bosonic particles have a modified equilibrium distribution function that implies a different influence on the evolution of the Universe that, in the case of massive neutrinos, can not be simply parametrized by a change in the effective number of neutrinos. Our results show that, despite the precision of the available cosmological data, only very weak bounds can be obtained on neutrino statistics, disfavouring a more bosonic behaviour at less than $2\sigma$., Comment: 18 pages, 9 figures
- Published
- 2018
- Full Text
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24. Model-Independent $\bar\nu_{e}$ Short-Baseline Oscillations from Reactor Spectral Ratios
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Gariazzo, S., Giunti, C., Laveder, M., and Li, Y. F.
- Subjects
High Energy Physics - Phenomenology ,High Energy Physics - Experiment ,Nuclear Experiment - Abstract
We consider the ratio of the spectra measured in the DANSS neutrino experiment at 12.7 and 10.7~m from a nuclear reactor. These data give a new model-independent indication in favor of short-baseline $\bar\nu_{e}$ oscillations which reinforce the model-independent indication found in the late 2016 in the NEOS experiment. The combined analysis of the NEOS and DANSS spectral ratios in the framework of 3+1 active-sterile neutrino mixing favor short-baseline $\bar\nu_{e}$ oscillations with a statistical significance of $3.7\sigma$. The two mixing parameters $\sin^{2}2\vartheta_{ee}$ and $\Delta{m}^{2}_{41}$ are constrained at $2\sigma$ in a narrow-$\Delta{m}^{2}_{41}$ island at $\Delta{m}^2_{41} \simeq 1.3 \, \text{eV}^2$, with $ \sin^{2}2\vartheta_{ee} = 0.049 \pm 0.023 $ ($2\sigma$). We discuss the implications of the model-independent NEOS+DANSS analysis for the reactor and Gallium anomalies. The NEOS+DANSS model-independent determination of short-baseline $\bar\nu_{e}$ oscillations allows us to analyze the reactor rates without assumptions on the values of the main reactor antineutrino fluxes and the data of the Gallium source experiments with free detector efficiencies. The corrections to the reactor neutrino fluxes and the Gallium detector efficiencies are obtained from the fit of the data. In particular, we confirm the indication in favor of the need for a recalculation of the $^{235}\text{U}$ reactor antineutrino flux found in previous studies assuming the absence of neutrino oscillations., Comment: 10 pages; analysis improved by taking into account the uncertainties of the reactor fission fractions
- Published
- 2018
- Full Text
- View/download PDF
25. Neutrino masses and their ordering: Global Data, Priors and Models
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Gariazzo, S., Archidiacono, M., de Salas, P. F., Mena, O., Ternes, C. A., and Tórtola, M.
- Subjects
High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
We present a Bayesian analysis of the combination of current neutrino oscillation, neutrinoless double beta decay and CMB observations. Our major goal is to carefully investigate the possibility to single out one neutrino mass ordering, Normal Ordering or Inverted Ordering, with current data. Two possible parametrizations (three neutrino masses versus the lightest neutrino mass plus the two oscillation mass splittings) and priors (linear versus logarithmic) are examined. We find that the preference for NO is only driven by neutrino oscillation data. Moreover, the values of the Bayes factor indicate that the evidence for NO is strong only when the scan is performed over the three neutrino masses with logarithmic priors; for every other combination of parameterization and prior, the preference for NO is only weak. As a by-product of our Bayesian analyses, we are able to a) compare the Bayesian bounds on the neutrino mixing parameters to those obtained by means of frequentist approaches, finding a very good agreement; b) determine that the lightest neutrino mass plus the two mass splittings parametrization, motivated by the physical observables, is strongly preferred over the three neutrino mass eigenstates scan and c) find that there is a weak-to-moderate preference for logarithmic priors. These results establish the optimal strategy to successfully explore the neutrino parameter space, based on the use of the oscillation mass splittings and a logarithmic prior on the lightest neutrino mass. We also show that the limits on the total neutrino mass $\sum m_\nu$ can change dramatically when moving from one prior to the other. These results have profound implications for future studies on the neutrino mass ordering, as they crucially state the need for self-consistent analyses which explore the best parametrization and priors, without combining results that involve different assumptions., Comment: 21 pages, 5 figures, 6 tables; Replaced to match version accepted for publication
- Published
- 2018
- Full Text
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26. Calculation of the local density of relic neutrinos
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de Salas, P. F., Gariazzo, S., Lesgourgues, J., and Pastor, S.
- Subjects
Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Nonzero neutrino masses are required by the existence of flavour oscillations, with values of the order of at least 50 meV. We consider the gravitational clustering of relic neutrinos within the Milky Way, and used the $N$-one-body simulation technique to compute their density enhancement factor in the neighbourhood of the Earth with respect to the average cosmic density. Compared to previous similar studies, we pushed the simulation down to smaller neutrino masses, and included an improved treatment of the baryonic and dark matter distributions in the Milky Way. Our results are important for future experiments aiming at detecting the cosmic neutrino background, such as the Princeton Tritium Observatory for Light, Early-universe, Massive-neutrino Yield (PTOLEMY) proposal. We calculate the impact of neutrino clustering in the Milky Way on the expected event rate for a PTOLEMY-like experiment. We find that the effect of clustering remains negligible for the minimal normal hierarchy scenario, while it enhances the event rate by 10 to 20% (resp. a factor 1.7 to 2.5) for the minimal inverted hierarchy scenario (resp. a degenerate scenario with 150 meV masses). Finally we compute the impact on the event rate of a possible fourth sterile neutrino with a mass of 1.3 eV., Comment: 24 pages, 5 figures. Matches published version
- Published
- 2017
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27. Updated Global 3+1 Analysis of Short-BaseLine Neutrino Oscillations
- Author
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Gariazzo, S., Giunti, C., Laveder, M., and Li, Y. F.
- Subjects
High Energy Physics - Phenomenology ,High Energy Physics - Experiment - Abstract
We present the results of an updated fit of short-baseline neutrino oscillation data in the framework of 3+1 active-sterile neutrino mixing. We first consider $\nu_e$ and $\bar\nu_e$ disappearance in the light of the Gallium and reactor anomalies. We discuss the implications of the recent measurement of the reactor $\bar\nu_e$ spectrum in the NEOS experiment, which shifts the allowed regions of the parameter space towards smaller values of $|U_{e4}|^2$. The beta-decay constraints allow us to limit the oscillation length between about 2 cm and 7 m at $3\sigma$ for neutrinos with an energy of 1 MeV. We then consider the global fit of the data in the light of the LSND anomaly, taking into account the constraints from $\nu_e$ and $\nu_\mu$ disappearance experiments, including the recent data of the MINOS and IceCube experiments. The combination of the NEOS constraints on $|U_{e4}|^2$ and the MINOS and IceCube constraints on $|U_{\mu4}|^2$ lead to an unacceptable appearance-disappearance tension which becomes tolerable only in a pragmatic fit which neglects the MiniBooNE low-energy anomaly. The minimization of the global $\chi^2$ in the space of the four mixing parameters $\Delta{m}^2_{41}$, $|U_{e4}|^2$, $|U_{\mu4}|^2$, and $|U_{\tau4}|^2$ leads to three allowed regions with narrow $\Delta{m}^{2}_{41}$ widths at $ \Delta m^2_{41} \approx 1.7 $ (best-fit), 1.3 (at $2\sigma$), 2.4 (at $3\sigma$) eV$^2$. The restrictions of the allowed regions of the mixing parameters with respect to our previous global fits are mainly due to the NEOS constraints. We present a comparison of the allowed regions of the mixing parameters with the sensitivities of ongoing experiments, which show that it is likely that these experiments will determine in a definitive way if the reactor, Gallium and LSND anomalies are due to active-sterile neutrino oscillations or not., Comment: 39 pages; improved treatment of the reactor flux uncertainties and other minor corrections
- Published
- 2017
- Full Text
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28. Light sterile neutrinos
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Gariazzo, S., Giunti, C., Laveder, M., Li, Y. F., and Zavanin, E. M.
- Subjects
High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment ,Physics - Accelerator Physics - Abstract
The theory and phenomenology of light sterile neutrinos at the eV mass scale is reviewed. The reactor, Gallium and LSND anomalies are briefly described and interpreted as indications of the existence of short-baseline oscillations which require the existence of light sterile neutrinos. The global fits of short-baseline oscillation data in 3+1 and 3+2 schemes are discussed, together with the implications for beta-decay and neutrinoless double-beta decay. The cosmological effects of light sterile neutrinos are briefly reviewed and the implications of existing cosmological data are discussed. The review concludes with a summary of future perspectives., Comment: 41 pages; final version to be published as a Topical Review in Journal of Physics G
- Published
- 2015
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29. Light Sterile Neutrinos and Inflationary Freedom
- Author
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Gariazzo, S., Giunti, C., and Laveder, M.
- Subjects
Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment ,High Energy Physics - Phenomenology - Abstract
We perform a cosmological analysis in which we allow the primordial power spectrum of scalar perturbations to assume a shape that is different from the usual power-law predicted by the simplest models of cosmological inflation. We parameterize the free primordial power spectrum with a "piecewise cubic Hermite interpolating polynomial" (PCHIP). We consider a 3+1 neutrino mixing model with a sterile neutrino having a mass at the eV scale, which can explain the anomalies observed in short-baseline neutrino oscillation experiments. We find that the freedom of the primordial power spectrum allows to reconcile the cosmological data with a fully thermalized sterile neutrino in the early Universe. Moreover, the cosmological analysis gives us some information on the shape of the primordial power spectrum, which presents a feature around the wavenumber $k=0.002\,\text{Mpc}^{-1}$., Comment: 19 pages; corrected Fig.4 and added Ref.[35]
- Published
- 2014
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30. Cosmological Invisible Decay of Light Sterile Neutrinos
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Gariazzo, S., Giunti, C., and Laveder, M.
- Subjects
Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment ,High Energy Physics - Phenomenology - Abstract
We introduce a cosmological invisible decay of the sterile neutrino with the eV-scale mass indicated by short-baseline neutrino oscillation experiments in order to allow its full thermalization in the early Universe. We show that the fit of the cosmological data is practically as good as the fit obtained with a stable sterile neutrino without mass constraints, which has been recently considered by several authors for the explanation of the observed suppression of small-scale matter density fluctuations and for a solution of the tension between the Planck and BICEP2 measurements of the tensor to scalar ratio of large-scale fluctuations. Moreover, the extra relativistic degree of freedom corresponding to a fully thermalized sterile neutrino is correlated with a larger value of the Hubble constant, which is in agreement with local measurements., Comment: 5 pages
- Published
- 2014
31. Light Sterile Neutrinos in Cosmology and Short-Baseline Oscillation Experiments
- Author
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Gariazzo, S., Giunti, C., and Laveder, M.
- Subjects
High Energy Physics - Phenomenology ,Astrophysics - Cosmology and Nongalactic Astrophysics ,High Energy Physics - Experiment - Abstract
We analyze the most recent cosmological data, including Planck, taking into account the possible existence of a sterile neutrino with a mass at the eV scale indicated by short-baseline neutrino oscillations data in the 3+1 framework. We show that the contribution of local measurements of the Hubble constant induces an increase of the value of the effective number of relativistic degrees of freedom above the Standard Model value, giving an indication in favor of the existence of sterile neutrinos and their contribution to dark radiation. Furthermore, the measurements of the local galaxy cluster mass distribution favor the existence of sterile neutrinos with eV-scale masses, in agreement with short-baseline neutrino oscillations data. In this case there is no tension between cosmological and short-baseline neutrino oscillations data, but the contribution of the sterile neutrino to the effective number of relativistic degrees of freedom is likely to be smaller than one. Considering the Dodelson-Widrow and thermal models for the statistical cosmological distribution of sterile neutrinos, we found that in the Dodelson-Widrow model there is a slightly better compatibility between cosmological and short-baseline neutrino oscillations data and the required suppression of the production of sterile neutrinos in the early Universe is slightly smaller., Comment: 12 pages; final version published in JHEP 1311 (2013) 211
- Published
- 2013
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32. Non-standard cosmic expansion histories: neutrino decoupling and primordial nucleosynthesis signatures
- Author
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Aristizabal Sierra, D., primary, Gariazzo, S., additional, and Villanueva, A., additional
- Published
- 2023
- Full Text
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33. Implementation and optimization of the PTOLEMY transverse drift electromagnetic filter
- Author
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Apponi, A, Betti, M, Borghesi, M, Canci, N, Cavoto, G, Chang, C, Chung, W, Cocco, A, Colijn, A, D'Ambrosio, N, De Groot, N, Faverzani, M, Ferella, A, Ferri, E, Ficcadenti, L, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Hochberg, Y, Kahn, Y, Kievsky, A, Lisanti, M, Mangano, G, Marcucci, L, Mariani, C, Messina, M, Monticone, E, Nucciotti, A, Orlandi, D, Pandolfi, F, Parlati, S, Perez De Los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Rago, I, Raitses, Y, Rajteri, M, Rossi, N, Rozwadowska, K, Ruocco, A, Strid, C, Tan, A, Tully, C, Viviani, M, Zeitler, U, Zhao, F, Apponi A., Betti M. G., Borghesi M., Canci N., Cavoto G., Chang C., Chung W., Cocco A. G., Colijn A. P., D'Ambrosio N., De Groot N., Faverzani M., Ferella A., Ferri E., Ficcadenti L., Gariazzo S., Gatti F., Gentile C., Giachero A., Hochberg Y., Kahn Y., Kievsky A., Lisanti M., Mangano G., Marcucci L. E., Mariani C., Messina M., Monticone E., Nucciotti A., Orlandi D., Pandolfi F., Parlati S., Perez De Los Heros C., Pisanti O., Polosa A. D., Puiu A., Rago I., Raitses Y., Rajteri M., Rossi N., Rozwadowska K., Ruocco A., Strid C. F., Tan A., Tully C. G., Viviani M., Zeitler U., Zhao F., Apponi, A, Betti, M, Borghesi, M, Canci, N, Cavoto, G, Chang, C, Chung, W, Cocco, A, Colijn, A, D'Ambrosio, N, De Groot, N, Faverzani, M, Ferella, A, Ferri, E, Ficcadenti, L, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Hochberg, Y, Kahn, Y, Kievsky, A, Lisanti, M, Mangano, G, Marcucci, L, Mariani, C, Messina, M, Monticone, E, Nucciotti, A, Orlandi, D, Pandolfi, F, Parlati, S, Perez De Los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Rago, I, Raitses, Y, Rajteri, M, Rossi, N, Rozwadowska, K, Ruocco, A, Strid, C, Tan, A, Tully, C, Viviani, M, Zeitler, U, Zhao, F, Apponi A., Betti M. G., Borghesi M., Canci N., Cavoto G., Chang C., Chung W., Cocco A. G., Colijn A. P., D'Ambrosio N., De Groot N., Faverzani M., Ferella A., Ferri E., Ficcadenti L., Gariazzo S., Gatti F., Gentile C., Giachero A., Hochberg Y., Kahn Y., Kievsky A., Lisanti M., Mangano G., Marcucci L. E., Mariani C., Messina M., Monticone E., Nucciotti A., Orlandi D., Pandolfi F., Parlati S., Perez De Los Heros C., Pisanti O., Polosa A. D., Puiu A., Rago I., Raitses Y., Rajteri M., Rossi N., Rozwadowska K., Ruocco A., Strid C. F., Tan A., Tully C. G., Viviani M., Zeitler U., and Zhao F.
- Published
- 2022
34. High Energy Physics Opportunities Using Reactor Antineutrinos
- Author
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Awe, C., Barbeau, P. S., Haghighat, A., Huber, P., Li, S. C., Link, J. M., Mascolino, V., Subedi, T., Walkup, K., Aguilar-Arevalo, A., Bertou, X., Bonifazi, C., Cancelo, G., Cervantes-Vergara, B. A., Chavez, C., D Olivo, J. C., Egea, J. M., Dos Anjos, J. C., Estrada, J., Neto, A. R. F., Fernandez-Moroni, G., Foguel, A., Ford, R., Gasanego, J., Gollo, V., Izraelevitch, F., Kilminster, B., Lima, Jr H. P., Makler, M., Mendes, L. H., Molina, J., Mota, P., Nasteva, I., Paolini, E., Romero, C., Sarkis, Y., Haro, M. S., Soto, A., Stalder, D., Tiffenberg, J., Torres, C., Lindner, M., An, F. P., Balantekin, A. B., Band, H. R., Bishai, M., Blyth, S., Cao, G. F., Cao, J., Chang, J. F., Chang, Y., Chen, H. S., Chen, S. M., Chen, Y., Chen, Y. X., Cheng, J., Cheng, Z. K., Cherwinka, J. J., Chu, M. C., Cummings, J. P., Dalager, O., Deng, F. S., Ding, Y. Y., Diwan, M. V., Dohnal, T., Dove, J., Dvořák, M., Dwyer, D. A., Gallo, J. P., Gonchar, M., Gong, G. H., Gong, H., Gu, W. Q., Guo, J. Y., Guo, L., Guo, X. H., Guo, Y. H., Guo, Z., Hackenburg, R. W., Hans, S., He, M., Heeger, K. M., Heng, Y. K., Higuera, A., Hor, Y. K., Hsiung, Y. B., Hu, B. Z., Hu, J. R., Hu, T., Hu, Z. J., Huang, H. X., Huang, X. T., Jaffe, D. E., Jen, K. L., Ji, X. L., Ji, X. P., Johnson, R. A., Jones, D., Kang, L., Kettell, S. H., Kohn, S., Kramer, M., Langford, T. J., Lee, J., Lee, J. H. C., Lei, R. T., Leitner, R., Leung, J. K. C., Li, F., Li, H. L., Li, J. J., Li, Q. J., Li, S., Li, W. D., Li, X. N., Li, X. Q., Li, Y. F., Li, Z. B., Liang, H., Lin, C. J., Lin, G. L., Lin, S., Ling, J. J., Littenberg, L., Littlejohn, B. R., Liu, J. C., Liu, J. L., Lu, C., Lu, H. Q., Lu, J. S., Luk, K. B., Ma, X. B., Ma, X. Y., Ma, Y. Q., Mandujano, R. C., Marshall, C., Martinez Caicedo, D. A., Mcdonald, K. T., Mckeown, R. D., Meng, Y., Napolitano, J., Naumov, D., Naumova, E., Ochoa-Ricoux, J. P., Olshevskiy, A., Pan, H. -R, Park, J., Patton, S., Peng, J. C., Pun, C. S. J., Qi, F. Z., Qi, M., Qian, X., Raper, N., Ren, J., Reveco, C. Morales, Rosero, R., Roskovec, B., Ruan, X. C., Steiner, H., Sun, J. L., Tmej, T., Treskov, K., Tse, W. -H, Tull, C. E., Viren, B., Vorobel, V., Wang, C. H., Wang, J., Wang, M., Wang, N. Y., Wang, R. G., Wang, W., Wang, X., Wang, Y., Wang, Y. F., Wang, Z., Wang, Z. M., Wei, H. Y., Wei, L. H., Wen, L. J., Whisnant, K., White, C. G., Wong, H. L. H., Worcester, E., Wu, D. R., Wu, F. L., Wu, Q., Wenjie Wu, Xia, D. M., Xie, Z. Q., Xing, Z. Z., Xu, J. L., Xu, T., Xue, T., Yang, C. G., Yang, L., Yang, Y. Z., Yao, H. F., Ye, M., Yeh, M., Young, B. L., Yu, H. Z., Yu, Z. Y., Yue, B. B., Zeng, S., Zeng, Y., Zhan, L., Zhang, C., Zhang, F. Y., Zhang, H. H., Zhang, J. W., Zhang, Q. M., Zhang, X. T., Zhang, Y. M., Zhang, Y. X., Zhang, Y. Y., Zhang, Z. J., Zhang, Z. P., Zhang, Z. Y., Zhao, J., Zhou, L., Zhuang, H. L., Zou, J. H., Abusleme, A., Adam, T., Ahmad, S., Ahmed, R., Aiello, S., An, G. P., An, Q., Andronico, G., Anfimov, N., Antonelli, V., Antoshkina, T., Asavapibhop, B., André, J. P. A. M., Auguste, D., Babic, A., Baldini, W., Barresi, A., Baussan, E., Bellato, M., Bergnoli, A., Bernieri, E., Birkenfeld, T., Blin, S., Blum, D., Bolshakova, A., Bongrand, M., Bordereau, C., Breton, D., Brigatti, A., Brugnera, R., Bruno, R., Budano, A., Buesken, M., Buscemi, M., Busto, Jose, Butorov, I., Cabrera, A., Cai, H., Cai, X., Cai, Y. K., Cai, Z. Y., Cammi, A., Campeny, A., Cao, C. Y., Caruso, R., Cerna, C., Chakaberia, I., Chen, P. P., Chen, P. A., Chen, S., Chen, X., Chen, Y. W., Chen, Z., Cheng, Y., Chiesa, D., Chimenti, P., Chukanov, A., Chuvashova, A., Claverie, G., Clementi, C., Clerbaux, B., Di Lorenzo, S., Corti, D., Costa, S., Corso, F. D., La Taille, C., Deng, J., Deng, Z., Deng, Z. Y., Depnering, W., Diaz, M., Ding, X. F., Dirgantara, B., Dmitrievsky, S., Donchenko, G., Dong, J. M., Dornic, D., Doroshkevich, E., Dracos, M., Druillole, F., Du, S. X., Dusini, S., Dvorak, M., Enqvist, T., Enzmann, H., Fabbri, A., Fajt, L., Fan, D. H., Fan, L., Fang, C., Fang, J., Fang, W. X., Fargetta, M., Fatkina, A., Fedoseev, D., Fekete, V., Feng, L. C., Feng, Q. C., Formozov, A., Fournier, A., Gan, H. N., Gao, F., Garfagnini, A., Göttel, A., Genster, C., Giammarchi, M., Giaz, A., Giudice, N., Gong, G., Gorchakov, O., Gornushkin, Y., Grassi, M., Grewing, C., Gromov, V., Gu, M., Gu, X., Gu, Y., Guan, M. Y., Guardone, N., Gul, M., Guo, C., Guo, W. L., Hackspacher, P., Hagner, C., Han, R., Han, Y., Hassan, M., He, W., Heinz, T., Hellmuth, P., Herrera, R., Hong, D. J., Hou, S. J., Hsiung, Y., Hu, H., Hu, J., Hu, S. Y., Huang, C. H., Huang, G. H., Huang, Q. H., Huang, W. H., Huang, X., Huang, Y. B., Hui, J. Q., Huo, L., Huo, W., Huss, C., Hussain, S., Insolia, A., Ioannisian, A., Isocrate, R., Ji, X. Z., Jia, H. H., Jia, J. J., Jian, S. Y., Jiang, D., Jiang, X. S., Jin, R. Y., Jing, X. P., Jollet, C., Joutsenvaara, J., Jungthawan, S., Kalousis, L., Kampmann, P., Karagounis, M., Kazarian, N., Khan, A., Khan, W., Khosonthongkee, K., Kinz, P., Korablev, D., Kouzakov, K., Krasnoperov, A., Krumshteyn, Z., Kruth, A., Kutovskiy, N., Kuusiniemi, P., Lachenmaier, T., Landini, C., Leblanc, S., Lebrin, V., Lefevre, F., Lei, R., Leung, J., Li, C., Li, D., Li, H., Li, J., Li, K. J., Li, M. Z., Li, M., Li, N., Li, R. H., Li, S. F., Li, S. J., Li, T., Li, W. G., Li, X. M., Li, X. L., Li, Y., Li, Z., Li, Z. Y., Liang, J. J., Liebau, D., Limphirat, A., Limpijumnong, S., Lin, S. X., Lin, T., Lippi, I., Liu, F., Liu, H. D., Liu, H. B., Liu, H. J., Liu, H. T., Liu, H., Liu, M., Liu, Q., Liu, R. X., Liu, S. Y., Liu, S. B., Liu, S. L., Liu, X. W., Liu, X., Liu, Y., Lokhov, A., Lombardi, P., Lombardo, C., Loo, K., Lu, J. B., Lu, J. G., Lu, S. X., Lu, X. X., Lubsandorzhiev, B., Lubsandorzhiev, S., Ludhova, L., Luo, F. J., Luo, G., Luo, P. W., Luo, S., Luo, W. M., Lyashuk, V., Ma, Q. M., Ma, S., Maalmi, J., Malyshkin, Y., Mantovani, F., Manzali, F., Mao, X., Mao, Y. J., Mari, S. M., Marini, F., Marium, S., Martellini, C., Martin-Chassard, G., Martini, A., Mayilyan, D., Müller, A., Mednieks, I., Meregaglia, A., Meroni, E., Meyhöfer, D., Mezzetto, M., Miller, J., Miramonti, L., Monforte, S., Montini, P., Montuschi, M., Morozov, N., Muhammad, A., Muralidharan, P., Nastasi, M., Naumov, D. V., Nemchenok, I., Ning, F. P., Ning, Z., Nunokawa, H., Oberauer, L., Orestano, D., Ortica, F., Pan, H. R., Paoloni, A., Parkalian, N., Parmeggiano, S., Payupol, T., Pei, Y., Pelliccia, N., Peng, A., Peng, H., Perrot, F., Petitjean, P. A., Petrucci, F., Piñeres Rico, L. F., Pilarczyk, O., Popov, A., Poussot, P., Pratumwan, W., Previtali, E., Qi, F., Qian, S., Qian, X. H., Qiao, H., Qin, Z. H., Qiu, S. K., Rajput, M., Ranucci, G., Re, A., Rebber, H., Rebii, A., Ren, B., Rezinko, T., Ricci, B., Robens, M., Roche, M., Rodphai, N., Romani, A., Roth, C., Ruan, X., Rujirawat, S., Rybnikov, A., Sadovsky, A., Saggese, P., Salamanna, G., Sanfilippo, S., Sangka, A., Sanguansak, N., Sawangwit, U., Sawatzki, J., Sawy, F., Schever, M., Schuler, J., Schwab, C., Schweizer, K., Selivanov, D., Selyunin, A., Serafini, A., Settanta, G., Settimo, M., Shao, Z., Sharov, V., Shi, J., Shutov, V., Sidorenkov, A., Simkovic, F., Sirignano, C., Siripak, J., Sisti, M., Slupecki, M., Smirnov, M., Smirnov, O., Sogo-Bezerra, T., Songwadhana, J., Soonthornthum, B., Sotnikov, A., Sramek, O., Sreethawong, W., Stahl, A., Stanco, L., Stankevich, K., Stefanik, D., Steiger, H., Steinmann, J., Sterr, T., Stock, M. R., Strati, V., Studenikin, A., Sun, G. X., Sun, S. F., Sun, X. L., Sun, Y. J., Sun, Y. Z., Suwonjandee, N., Szelezniak, M., Tang, J., Tang, Q., Tang, X., Tietzsch, A., Tkachev, I., Triossi, A., Troni, G., Trzaska, W., Tuve, C., Ushakov, N., Waasen, S., Boom, J. Vanden, Vanroyen, G., Vassilopoulos, N., Vedin, V., Verde, G., Vialkov, M., Viaud, B., Volpe, C., Voronin, D., Votano, L., Walker, P., Wang, C., Wang, E., Wang, G., Wang, K. Y., Wang, L., Wang, M. F., Wang, S. G., Wang, W. S., Wang, X. Y., Wang, Y. G., Wang, Y. Q., Wang, Z. Y., Waqas, M., Watcharangkool, A., Wei, W., Wei, Y. D., Wiebusch, C., Wong, S. C. F., Wonsak, B., Wu, D., Wu, W. J., Wu, Z., Wurm, M., Wurtz, J., Wysotzki, C., Xi, Y. F., Xie, Y. G., Xu, B., Xu, C., Xu, D. L., Xu, F. R., Xu, H. K., Xu, J., Xu, M. H., Xu, Y., Yan, B. J., Yan, T., Yan, W. Q., Yan, X. B., Yan, Y. P., Yang, A. B., Yang, H., Yang, J., Yang, X. Y., Yang, Y., Yang, Y. F., Yasin, Z., Ye, J. X., Ye, Z. P., Yegin, U., Yermia, F., Yi, P. H., Yin, X. W., You, Z. Y., Yu, B. X., Yu, C. Y., Yu, C. X., Yu, M., Yu, X. H., Yuan, C. Z., Yuan, Y., Yuan, Z. X., Yuan, Z. Y., Zafar, N., Zambanini, A., Zeng, T. X., Zeng, Y. D., Zhang, G. Q., Zhang, H. Q., Zhang, J., Zhang, J. B., Zhang, P., Zhang, S., Zhang, T., Zhang, X. M., Zhang, Y., Zhang, Y. H., Zhang, Y. P., Zhao, F. Y., Zhao, R., Zhao, S. J., Zhao, T. C., Zheng, D. Q., Zheng, H., Zheng, M. S., Zheng, Y. H., Zhong, W. R., Zhou, J., Zhou, N., Zhou, S., Zhou, X., Zhu, J., Zhu, K. J., Zhuang, B., Zong, L., Rasco, B. C., Han, B. Y., Jeon, E. J., Jeong, Y., Jo, H. S., Kim, D. K., Kim, J. Y., Kim, J. G., Kim, Y. D., Ko, Y. J., Lee, H. M., Lee, M. H., Moon, C. S., Oh, Y. M., Park, H. K., Park, K. S., Seo, S. H., Siyeon, K., Sun, G. M., Yoon, Y. S., Yu, I., Borusinski, M. J., Dorrill, R., Druetzler, A., Learned, J., Li, V., Markoff, D., Maricic, J., Matsuno, S., Mumm, H. P., Nishimura, K., Irani, A., Pitt, M., Rasco, C., Thibodeau, B., Varner, G., Vogelaar, B., Wright, T., Andriamirado, M., Bass, C. D., Bergeron, D. E., Berish, D., Bowden, N. S., Brodsky, J. P., Bryan, C. D., Carr, R., Classen, T., Conant, A. J., Deichert, G., Dolinski, M. J., Erickson, A., Foust, B. T., Gaison, J. K., Galindo-Uribarri, A., Gilbert, C. E., Grant, C., Hackett, B. T., Hansell, A. B., Ji, X., Jones, D. C., Kyzylova, O., Lane, C. E., Larosa, J., Lu, X., Mendenhall, M. P., Meyer, A. M., Milincic, R., Mitchell, I., Mueller, P. E., Nave, C., Neilson, R., Nikkel, J. A., Norcini, D., Nour, S., Palomino, J. L., Pushin, D. A., Romero-Romero, E., Surukuchi, P. T., Tyra, M. A., Varner, R. L., Venegas-Vargas, D., Weatherly, P. B., White, C., Wilhelmi, J., Woolverton, A., Zhang, A., Zhang, X., Choi, J. H., Jang, H. I., Jang, J. S., Jeon, S. H., Joo, K. K., Ju, K., Jung, D. E., Kim, J. H., Kim, S. B., Kim, S. Y., Kim, W., Kwon, E., Lee, D. H., Lee, H. G., Lim, I. T., Moon, D. H., Pac, M. Y., Seo, H., Seo, J. W., Shin, C. D., Yang, B. S., Yoo, J., Yoon, S. G., Yeo, I. S., Chang, C., Bergé, L., Broniatowski, A., Dumoulin, L., Giuliani, A., Chapellier, M., Marcillac, P., Marnieros, S., Olivieri, E., Poda, D., Calvo, M., Goupy, J., Monfardini, A., Arnaud, Q., Augier, C., Billard, J., Cazes, A., Colas, J., Filippini, J., Gascon, J., Jesus, M., Lattaud, H., Juillard, A., Salagnac, T., Soldner, T., Lubashevskiy, A., Yakushev, E., Rozov, S., Lamblin, J., Mom, B., Stutz, A., Formaggio, J. A., Mayer, D. W., Johnston, J., Harrington, P., Heine, S., Sibille, V., Chen, R., Figueroa-Feliciano, E., Ziqing, H., Hertel, S., Patel, P., Pinckney, D., Serafin, A., Shilcusky, A., Decheine, N., Palladino, K., Weber, S., Hirjibehedin, C., Akindele, O. A., Carman, L., Dazeley, S., Ford, M., Jovanovic, I., Sutanto, F., Zaitseva, N., Beaumont, W., Binet, S., Bolognino, I., Borg, J., Buridon, V., Chanal, H., Coupé, B., Crochet, P., Cussans, D., Roeck, A., Durand, D., Fallot, M., Galbinski, D., Gallego, S., Giot, L., Guillon, B., Henaff, D., Hayashida, S., Hosseini, B., Kalcheva, S., Lehaut, G., Michiels, I., Monteil, S., Newbold, D., Roy, N., Ryckbosch, D., Sfar, H. Rejeb, Simard, L., Vacheret, A., Vandierendonck, G., Dyck, S., Remortel, N., Vercaemer, S., Verstraeten, M., Weber, A., Yeresko, M., Bonhomme, A., Buck, C., Del Amo Sanchez, P., El Atmani, I., Labit, L., Letourneau, A., Lhuillier, D., Licciardi, M., Materna, T., Pessard, H., Rogly, R., Savu, V., Schoppmann, S., Vialat, M., Algora, A., Beloeuvre, A., Estienne, M., Kean, R., Porta, A., Tain, J. L., Sidelnik, I., Anderson, T., Askins, M., Bagdasarian, Z., Baldoni, A., Barna, A., Benson, T., Bergevin, M., Bernstein, A., Birrittella, B., Bogetic, S., Boissevain, J., Borusinki, J., Boyd, S., Brooks, T., Budsworth, Mat, Burns, J., Calle, M., Camilo, C., Carroll, A., Coleman, J., Collins, R., Connor, C., Cowen, D., Crow, B., Curry, J., Dalnoki-Veress, F., Danielson, D., Diwan, M., Dixon, S., Drakopoulou, L., Duron, J., Dye, S., Fargher, S., Fienberg, A., Fischer, V., Foster, R., Frankiewicz, Kat, Gamble, T., Gooding, D., Gokhale, S., Gregorio, R., Gribble, J., Griskevich, J., Hadley, D., He, J., Healey, K., Hecla, J., Holt, G., Jabbari, C., Jewkes, K., Kaiser, R., Keenan, M., Keener, P., Kneale, Liz, Kudryavtsev, V., Kunkle, P., Litchfield, P., Liu, X. Ran, Lynch, G., Malek, M., Marr-Laundrie, P., Masic, B., Mauger, C., Mccauley, N., Metelko, C., Mills, R., Mitra, A., Muheim, F., Mullen, A., Murphy, A., Needham, M., Neights, E., Ogren, K., Orebi Gann, G., Oxborough, L., Paling, S., Papatyi, A., Paulos, B., Pershing, T., Pickard, L., Quillin, S., Resoro, R., Richards, B., Sabarots, L., Scarff, A., Schnellbach, Yan-Jie, Scovell, P., Seitz, B., Shea, O., Shebalin, V., Smith, G., Smy, M., Song, H., Spooner, N., Stanton, C., Stone, O., Svoboda, R., Szoldos, S., Thompson, L., Thomson, F., Toth, C., Vagins, M., Berg, Rick, Ventura, S., Walsh, B., Webster, J., Weiss, M., Westphal, D., Wetstein, M., Wilson, T., Wilson, S., Wolcott, S., Wright, M., Berryman, J. M., Collar, J. I., Erlandson, A., Gariazzo, S., Garzelli, M. V., Giunti, C., Goldblum, B. L., Hayes, A., Hedges, S., Mariani, C., Minic, D., Mougeot, X., Naim, D., Newby, J., Ni, K., O Donnell, T., Ozturk, S., Périssé, L., Pestes, R., Sonzogni, A. A., Tabrizi, Z., Vivier, M., Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Neutrino de Champagne Ardenne (LNCA - UMS 3263), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de physique subatomique et des technologies associées (SUBATECH), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-IMT Atlantique (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT)-Nantes université - UFR des Sciences et des Techniques (Nantes univ - UFR ST), Nantes Université - pôle Sciences et technologie, Nantes Université (Nantes Univ)-Nantes Université (Nantes Univ)-Nantes Université - pôle Sciences et technologie, Nantes Université (Nantes Univ)-Nantes Université (Nantes Univ), Centre de Sciences Nucléaires et de Sciences de la Matière (CSNSM), Cryogénie (NEEL - Cryo), Institut Néel (NEEL), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Hélium : du fondamental aux applications (NEEL - HELFA), Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de l'Accélérateur Linéaire (LAL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Institut Laue-Langevin (ILL), Laboratoire d'Intégration des Systèmes et des Technologies (LIST (CEA)), Direction de Recherche Technologique (CEA) (DRT (CEA)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Département de Physique Nucléaire (ex SPhN) (DPHN), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, CHANDLER, CONNIE, CONUS, Daya Bay, JUNO, MTAS, NEOS, NuLat, PROSPECT, RENO, Ricochet, ROADSTR Near-Field Working Group, SoLid, Stereo, Valencia-Nantes TAGS, vIOLETA, WATCHMAN, and HEP, INSPIRE
- Subjects
High Energy Physics - Experiment (hep-ex) ,[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex] ,hep-ex ,neutrino: energy spectrum ,antineutrino: nuclear reactor ,[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] ,FOS: Physical sciences ,neutrino: oscillation ,neutrino: nuclear reactor ,Particle Physics - Experiment ,neutrino: flux ,High Energy Physics - Experiment - Abstract
Nuclear reactors are uniquely powerful, abundant, and flavor-pure sources of antineutrinos that continue to play a vital role in the US neutrino physics program. The US reactor antineutrino physics community is a diverse interest group encompassing many detection technologies and many particle physics topics, including Standard Model and short-baseline oscillations, BSM physics searches, and reactor flux and spectrum modeling. The community's aims offer strong complimentary with numerous aspects of the wider US neutrino program and have direct relevance to most of the topical sub-groups composing the Snowmass 2021 Neutrino Frontier. Reactor neutrino experiments also have a direct societal impact and have become a strong workforce and technology development pipeline for DOE National Laboratories and universities. This white paper, prepared as a submission to the Snowmass 2021 community organizing exercise, will survey the state of the reactor antineutrino physics field and summarize the ways in which current and future reactor antineutrino experiments can play a critical role in advancing the field of particle physics in the next decade., Contribution to Snowmass 2021
- Published
- 2022
35. Implementation and optimization of the PTOLEMY transverse drift electromagnetic filter
- Author
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Apponi, A., Betti, M. G., Borghesi, M., Canci, N., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., D'Ambrosio, N., de Groot, N., Faverzani, M., Ferella, A., Ferri, E., Ficcadenti, L., Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Hochberg, Y., Kahn, Y., Kievsky, A., Lisanti, M., Mangano, G., Marcucci, L. E., Mariani, C., Messina, M., Monticone, E., Nucciotti, A., Orlandi, D., Pandolfi, F., Parlati, S., Pérez de los Heros, Carlos, Pisanti, O., Polosa, A. D., Puiu, A., Rago, I, Raitses, Y., Rajteri, M., Rossi, N., Rozwadowska, K., Ruocco, A., Strid, C. F., Tan, A., Tully, C. G., Viviani, M., Zeitler, U., Zhao, F., Apponi, A., Betti, M. G., Borghesi, M., Canci, N., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., D'Ambrosio, N., de Groot, N., Faverzani, M., Ferella, A., Ferri, E., Ficcadenti, L., Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Hochberg, Y., Kahn, Y., Kievsky, A., Lisanti, M., Mangano, G., Marcucci, L. E., Mariani, C., Messina, M., Monticone, E., Nucciotti, A., Orlandi, D., Pandolfi, F., Parlati, S., Pérez de los Heros, Carlos, Pisanti, O., Polosa, A. D., Puiu, A., Rago, I, Raitses, Y., Rajteri, M., Rossi, N., Rozwadowska, K., Ruocco, A., Strid, C. F., Tan, A., Tully, C. G., Viviani, M., Zeitler, U., and Zhao, F.
- Abstract
The PTOLEMY transverse drift filter is a new concept to enable precision analysis of the energy spectrum of electrons near the tritium beta-decay endpoint. This paper details the implementation and optimization methods for successful operation of the filter for electrons with a known pitch angle. We present the first demonstrator that produces the required magnetic field properties with an iron return-flux magnet. Two methods for the setting of filter electrode voltages are detailed. The challenges of low-energy electron transport in cases of low field are discussed, such as the growth of the cyclotron radius with decreasing magnetic field, which puts a ceiling on filter performance relative to fixed filter dimensions. Additionally, low pitch angle trajectories are dominated by motion parallel to the magnetic field lines and introduce non-adiabatic conditions and curvature drift. To minimize these effects and maximize electron acceptance into the filter, we present a three-potential-well design to simultaneously drain the parallel and transverse kinetic energies throughout the length of the filter. These optimizations are shown, in simulation, to achieve low-energy electron transport from a 1 T iron core (or 3 T superconducting) starting field with initial kinetic energy of 18.6 keV drained to < 10 eV (< 1 eV) in about 80 cm. This result for low field operation paves the way for the first demonstrator of the PTOLEMY spectrometer for measurement of electrons near the tritium endpoint to be constructed at the Gran Sasso National Laboratory (LNGS) in Italy.
- Published
- 2022
- Full Text
- View/download PDF
36. Implementation and optimization of the PTOLEMY transverse drift electromagnetic filter
- Author
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Apponi, A., primary, Betti, M.G., additional, Borghesi, M., additional, Canci, N., additional, Cavoto, G., additional, Chang, C., additional, Chung, W., additional, Cocco, A.G., additional, Colijn, A.P., additional, D'Ambrosio, N., additional, de Groot, N., additional, Faverzani, M., additional, Ferella, A., additional, Ferri, E., additional, Ficcadenti, L., additional, Gariazzo, S., additional, Gatti, F., additional, Gentile, C., additional, Giachero, A., additional, Hochberg, Y., additional, Kahn, Y., additional, Kievsky, A., additional, Lisanti, M., additional, Mangano, G., additional, Marcucci, L.E., additional, Mariani, C., additional, Messina, M., additional, Monticone, E., additional, Nucciotti, A., additional, Orlandi, D., additional, Pandolfi, F., additional, Parlati, S., additional, Pérez de los Heros, C., additional, Pisanti, O., additional, Polosa, A.D., additional, Puiu, A., additional, Rago, I., additional, Raitses, Y., additional, Rajteri, M., additional, Rossi, N., additional, Rozwadowska, K., additional, Ruocco, A., additional, Strid, C.F., additional, Tan, A., additional, Tully, C.G., additional, Viviani, M., additional, Zeitler, U., additional, and Zhao, F., additional
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- 2022
- Full Text
- View/download PDF
37. PArthENoPE revolutions
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Gariazzo, S., primary, F. de Salas, P., additional, Pisanti, O., additional, and Consiglio, R., additional
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- 2022
- Full Text
- View/download PDF
38. A design for an electromagnetic filter for precision energy measurements at the tritium endpoint
- Author
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Betti, M, Biasotti, M, Boscá, A, Calle, F, Carabe-Lopez, J, Cavoto, G, Chang, C, Chung, W, Cocco, A, Colijn, A, Conrad, J, D’Ambrosio, N, de Salas, P, Faverzani, M, Ferella, A, Ferri, E, Garcia-Abia, P, Gomez-Tejedor, G, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Gudmundsson, J, Hochberg, Y, Kahn, Y, Lisanti, M, Mancini-Terracciano, C, Mangano, G, Marcucci, L, Mariani, C, Martínez, J, Messina, M, Molinero-Vela, A, Monticone, E, Nucciotti, A, Pandolfi, F, Pastor, S, Pedrós, J, de los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Raitses, Y, Rajteri, M, Rossi, N, Santorelli, R, Schaeffner, K, Strid, C, Tully, C, Zhao, F, Zurek, K, Betti, M. G., Biasotti, M., Boscá, A., Calle, F., Carabe-Lopez, J., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., Conrad, J., D’Ambrosio, N., de Salas, P. F., Faverzani, M., Ferella, A., Ferri, E., Garcia-Abia, P., Gomez-Tejedor, G. Garcia, Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Gudmundsson, J. E., Hochberg, Y., Kahn, Y., Lisanti, M., Mancini-Terracciano, C., Mangano, G., Marcucci, L. E., Mariani, C., Martínez, J., Messina, M., Molinero-Vela, A., Monticone, E., Nucciotti, A., Pandolfi, F., Pastor, S., Pedrós, J., de los Heros, C. Pérez, Pisanti, O., Polosa, A. D., Puiu, A., Raitses, Y., Rajteri, M., Rossi, N., Santorelli, R., Schaeffner, K., Strid, C. F., Tully, C. G., Zhao, F., Zurek, K. M., Betti, M, Biasotti, M, Boscá, A, Calle, F, Carabe-Lopez, J, Cavoto, G, Chang, C, Chung, W, Cocco, A, Colijn, A, Conrad, J, D’Ambrosio, N, de Salas, P, Faverzani, M, Ferella, A, Ferri, E, Garcia-Abia, P, Gomez-Tejedor, G, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Gudmundsson, J, Hochberg, Y, Kahn, Y, Lisanti, M, Mancini-Terracciano, C, Mangano, G, Marcucci, L, Mariani, C, Martínez, J, Messina, M, Molinero-Vela, A, Monticone, E, Nucciotti, A, Pandolfi, F, Pastor, S, Pedrós, J, de los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Raitses, Y, Rajteri, M, Rossi, N, Santorelli, R, Schaeffner, K, Strid, C, Tully, C, Zhao, F, Zurek, K, Betti, M. G., Biasotti, M., Boscá, A., Calle, F., Carabe-Lopez, J., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., Conrad, J., D’Ambrosio, N., de Salas, P. F., Faverzani, M., Ferella, A., Ferri, E., Garcia-Abia, P., Gomez-Tejedor, G. Garcia, Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Gudmundsson, J. E., Hochberg, Y., Kahn, Y., Lisanti, M., Mancini-Terracciano, C., Mangano, G., Marcucci, L. E., Mariani, C., Martínez, J., Messina, M., Molinero-Vela, A., Monticone, E., Nucciotti, A., Pandolfi, F., Pastor, S., Pedrós, J., de los Heros, C. Pérez, Pisanti, O., Polosa, A. D., Puiu, A., Raitses, Y., Rajteri, M., Rossi, N., Santorelli, R., Schaeffner, K., Strid, C. F., Tully, C. G., Zhao, F., and Zurek, K. M.
- Abstract
We present a detailed description of the electromagnetic filter for the PTOLEMY project to directly detect the Cosmic Neutrino Background (CNB). Starting with an initial estimate for the orbital magnetic moment, the higher-order drift process of E×B is configured to balance the gradient-B drift motion of the electron in such a way as to guide the trajectory into the standing voltage potential along the mid-plane of the filter. As a function of drift distance along the length of the filter, the filter zooms in with exponentially increasing precision on the transverse velocity component of the electron kinetic energy. This yields a linear dimension for the total filter length that is exceptionally compact compared to previous techniques for electromagnetic filtering. The parallel velocity component of the electron kinetic energy oscillates in an electrostatic harmonic trap as the electron drifts along the length of the filter. An analysis of the phase-space volume conservation validates the expected behavior of the filter from the adiabatic invariance of the orbital magnetic moment and energy conservation following Liouville's theorem for Hamiltonian systems.
- Published
- 2019
39. Neutrino physics with the PTOLEMY project: Active neutrino properties and the light sterile case
- Author
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Betti, M, Biasotti, M, Bosca, A, Calle, F, Canci, N, Cavoto, G, Chang, C, Cocco, A, Colijn, A, Conrad, J, D'Ambrosio, N, De Groot, N, De Salas, P, Faverzani, M, Ferella, A, Ferri, E, Garcia-Abia, P, Garcia-Cortes, I, Gomez-Tejedor, G, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Gudmundsson, J, Hochberg, Y, Kahn, Y, Kievsky, A, Lisanti, M, Mancini-Terracciano, C, Mangano, G, Marcucci, L, Mariani, C, Martinez, J, Messina, M, Molinero-Vela, A, Monticone, E, Morono, A, Nucciotti, A, Pandolfi, F, Parlati, S, Pastor, S, Pedros, J, De Los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Rago, I, Raitses, Y, Rajteri, M, Rossi, N, Rucandio, I, Santorelli, R, Schaeffner, K, Tully, C, Viviani, M, Zhao, F, Zurek, K, Betti M. G., Biasotti M., Bosca A., Calle F., Canci N., Cavoto G., Chang C., Cocco A. G., Colijn A. P., Conrad J., D'Ambrosio N., De Groot N., De Salas P. F., Faverzani M., Ferella A., Ferri E., Garcia-Abia P., Garcia-Cortes I., Gomez-Tejedor G. G., Gariazzo S., Gatti F., Gentile C., Giachero A., Gudmundsson J. E., Hochberg Y., Kahn Y., Kievsky A., Lisanti M., Mancini-Terracciano C., Mangano G., Marcucci L. E., Mariani C., Martinez J., Messina M., Molinero-Vela A., Monticone E., Morono A., Nucciotti A., Pandolfi F., Parlati S., Pastor S., Pedros J., De Los Heros C. P., Pisanti O., Polosa A. D., Puiu A., Rago I., Raitses Y., Rajteri M., Rossi N., Rucandio I., Santorelli R., Schaeffner K., Tully C. G., Viviani M., Zhao F., Zurek K. M., Betti, M, Biasotti, M, Bosca, A, Calle, F, Canci, N, Cavoto, G, Chang, C, Cocco, A, Colijn, A, Conrad, J, D'Ambrosio, N, De Groot, N, De Salas, P, Faverzani, M, Ferella, A, Ferri, E, Garcia-Abia, P, Garcia-Cortes, I, Gomez-Tejedor, G, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Gudmundsson, J, Hochberg, Y, Kahn, Y, Kievsky, A, Lisanti, M, Mancini-Terracciano, C, Mangano, G, Marcucci, L, Mariani, C, Martinez, J, Messina, M, Molinero-Vela, A, Monticone, E, Morono, A, Nucciotti, A, Pandolfi, F, Parlati, S, Pastor, S, Pedros, J, De Los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Rago, I, Raitses, Y, Rajteri, M, Rossi, N, Rucandio, I, Santorelli, R, Schaeffner, K, Tully, C, Viviani, M, Zhao, F, Zurek, K, Betti M. G., Biasotti M., Bosca A., Calle F., Canci N., Cavoto G., Chang C., Cocco A. G., Colijn A. P., Conrad J., D'Ambrosio N., De Groot N., De Salas P. F., Faverzani M., Ferella A., Ferri E., Garcia-Abia P., Garcia-Cortes I., Gomez-Tejedor G. G., Gariazzo S., Gatti F., Gentile C., Giachero A., Gudmundsson J. E., Hochberg Y., Kahn Y., Kievsky A., Lisanti M., Mancini-Terracciano C., Mangano G., Marcucci L. E., Mariani C., Martinez J., Messina M., Molinero-Vela A., Monticone E., Morono A., Nucciotti A., Pandolfi F., Parlati S., Pastor S., Pedros J., De Los Heros C. P., Pisanti O., Polosa A. D., Puiu A., Rago I., Raitses Y., Rajteri M., Rossi N., Rucandio I., Santorelli R., Schaeffner K., Tully C. G., Viviani M., Zhao F., and Zurek K. M.
- Abstract
The PTOLEMY project aims to develop a scalable design for a Cosmic Neutrino Background (CNB) detector, the first of its kind and the only one conceived that can look directly at the image of the Universe encoded in neutrino background produced in the first second after the Big Bang. The scope of the work for the next three years is to complete the conceptual design of this detector and to validate with direct measurements that the non-neutrino backgrounds are below the expected cosmological signal. In this paper we discuss in details the theoretical aspects of the experiment and its physics goals. In particular, we mainly address three issues. First we discuss the sensitivity of PTOLEMY to the standard neutrino mass scale. We then study the perspectives of the experiment to detect the CNB via neutrino capture on tritium as a function of the neutrino mass scale and the energy resolution of the apparatus. Finally, we consider an extra sterile neutrino with mass in the eV range, coupled to the active states via oscillations, which has been advocated in view of neutrino oscillation anomalies. This extra state would contribute to the tritium decay spectrum, and its properties, mass and mixing angle, could be studied by analyzing the features in the beta decay electron spectrum.
- Published
- 2019
40. 2020 global reassessment of the neutrino oscillation picture
- Author
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de Salas, Pablo F., Forero, D., Gariazzo, S., Martínez-Miravé, P., Mena, O., Ternes, C. A., Tórtola, M., Valle, J. W. F., de Salas, Pablo F., Forero, D., Gariazzo, S., Martínez-Miravé, P., Mena, O., Ternes, C. A., Tórtola, M., and Valle, J. W. F.
- Abstract
We present an updated global fit of neutrino oscillation data in the simplest three-neutrino framework. In the present study we include up-to-date analyses from a number of experiments. Concerning the atmospheric and solar sectors, besides the data considered previously, we give updated analyses of IceCube DeepCore and Sudbury Neutrino Observatory data, respectively. We have also included the latest electron antineutrino data collected by the Daya Bay and RENO reactor experiments, and the long-baseline T2K and NO nu A measurements, as reported in the Neutrino 2020 conference. All in all, these new analyses result in more accurate measurements of theta (13), theta (12), Delta m212 and Delta m312. The best fit value for the atmospheric angle theta (23) lies in the second octant, but first octant solutions remain allowed at similar to 2.4 sigma. Regarding CP violation measurements, the preferred value of delta we obtain is 1.08 pi (1.58 pi) for normal (inverted) neutrino mass ordering. The global analysis still prefers normal neutrino mass ordering with 2.5 sigma statistical significance. This preference is milder than the one found in previous global analyses. These new results should be regarded as robust due to the agreement found between our Bayesian and frequentist approaches. Taking into account only oscillation data, there is a weak/moderate preference for the normal neutrino mass ordering of 2.00 sigma. While adding neutrinoless double beta decay from the latest Gerda, CUORE and KamLAND-Zen results barely modifies this picture, cosmological measurements raise the preference to 2.68 sigma within a conservative approach. A more aggressive data set combination of cosmological observations leads to a similar preference for normal with respect to inverted mass ordering, namely 2.70 sigma. This very same cosmological data set provides 2 sigma upper limits on the total neutrino mass corresponding to Sigma m(nu)< 0.12 (0.15) eV in the normal (inverted) neutrino mass
- Published
- 2021
- Full Text
- View/download PDF
41. Most constraining cosmological neutrino mass bounds
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Ministerio de Ciencia e Innovación (España), Di Valentino, Eleonora, Gariazzo, S., Mena, Olga, Ministerio de Ciencia e Innovación (España), Di Valentino, Eleonora, Gariazzo, S., and Mena, Olga
- Abstract
We present here up-to-date neutrino mass limits exploiting the most recent cosmological data sets. By making use of the cosmic microwave background temperature fluctuation and polarization measurements, supernovae Ia luminosity distances, baryon acoustic oscillation observations and determinations of the growth rate parameter, we are able to set the most constraining bound to date, at 95% C.L. This very tight limit is obtained without the assumption of any prior on the value of the Hubble constant and highly compromises the viability of the inverted mass ordering as the underlying neutrino mass pattern in nature. The results obtained here further strengthen the case for very large multitracer spectroscopic surveys as unique laboratories for cosmological relics, such as neutrinos: that would be the case of the Dark Energy Spectroscopic Instrument survey and of the Euclid mission.
- Published
- 2021
42. Model-independent ν¯e short-baseline oscillations from reactor spectral ratios
- Author
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Gariazzo, S., Giunti, C., Laveder, M., and Y. F., Li
- Subjects
High Energy Physics - Phenomenology ,Nuclear and High Energy Physics ,High Energy Physics - Experiment ,Nuclear Experiment ,lcsh:Physics ,lcsh:QC1-999 - Abstract
We consider the ratio of the spectra measured in the DANSS neutrino experiment at 12.7 and 10.7 m from a nuclear reactor. These data give a new model-independent indication in favor of short-baseline ν¯e oscillations which reinforce the model-independent indication found in the late 2016 in the NEOS experiment. The combined analysis of the NEOS and DANSS spectral ratios in the framework of 3+1 active–sterile neutrino mixing favor short-baseline ν¯e oscillations with a statistical significance of 3.7σ. The two mixing parameters sin22ϑee and Δm412 are constrained at 2σ in a narrow-Δm412 island at Δm412≃1.3eV2, with sin22ϑee=0.049±0.023 (2σ). We discuss the implications of the model-independent NEOS+DANSS analysis for the reactor and Gallium anomalies. The NEOS+DANSS model-independent determination of short-baseline ν¯e oscillations allows us to analyze the reactor rates without assumptions on the values of the main reactor antineutrino fluxes and the data of the Gallium source experiments with free detector efficiencies. The corrections to the reactor neutrino fluxes and the Gallium detector efficiencies are obtained from the fit of the data. In particular, we confirm the indication in favor of the need for a recalculation of the U235 reactor antineutrino flux found in previous studies assuming the absence of neutrino oscillations.
- Published
- 2018
43. 2020 global reassessment of the neutrino oscillation picture
- Author
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de Salas, P. F., primary, Forero, D. V., additional, Gariazzo, S., additional, Martínez-Miravé, P., additional, Mena, O., additional, Ternes, C. A., additional, Tórtola, M., additional, and Valle, J. W. F., additional
- Published
- 2021
- Full Text
- View/download PDF
44. Constraining power of open likelihoods, made prior-independent
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Gariazzo, S., primary
- Published
- 2020
- Full Text
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45. Neutrino masses, states and interactions: Session summary
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Gariazzo, S, Sisti, M, Gariazzo S., Sisti M., Gariazzo, S, Sisti, M, Gariazzo S., and Sisti M.
- Abstract
In these proceedings we present a brief summary of the parallel Session IV, “Neutrino masses, states and interactions”, part of the Neutrino Oscillation Workshop 2018∗. Topics of the session included the current status of some experimental searches for the neutrino absolute mass scale, a resume of recent results and developments in neutrinoless double beta decay, the situation of the search for a light sterile neutrino with a mass around 1 eV, a phenomenological summary on neutrino electromagnetic properties and a discussion about theoretical models for neutrino masses and mixings.
- Published
- 2018
46. Neutrino clustering in the Milky Way and beyond
- Author
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Mertsch, P., Parimbelli, G., de Salas, Pablo Fernández, Gariazzo, S., Lesgourgues, J., Pastor, S., Mertsch, P., Parimbelli, G., de Salas, Pablo Fernández, Gariazzo, S., Lesgourgues, J., and Pastor, S.
- Abstract
The standard cosmological model predicts the existence of a Cosmic Neutrino Background, which has not yet been observed directly. Some experiments aiming at its detection are currently under development, despite the tiny kinetic energy of the cosmological relic neutrinos, which makes this task incredibly challenging. Since massive neutrinos are attracted by the gravitational potential of our Galaxy, they can cluster locally. Neutrinos should be more abundant at the Earth position than at an average point in the Universe. This fact may enhance the expected event rate in any future experiment. Past calculations of the local neutrino clustering factor only considered a spherical distribution of matter in the Milky Way and neglected the influence of other nearby objects like the Virgo cluster, although recent N-body simulations suggest that the latter may actually be important. In this paper, we adopt a back-tracking technique, well established in the calculation of cosmic rays fluxes, to perform the first three-dimensional calculation of the number density of relic neutrinos at the Solar System, taking into account not only the matter composition of the Milky Way, but also the contribution of the Andromeda galaxy and the Virgo cluster. The effect of Virgo is indeed found to be relevant and to depend non-trivially on the value of the neutrino mass. Our results show that the local neutrino density is enhanced by 0.53% for a neutrino mass of 10 meV, 12% for 50 meV, 50% for 100 meV or 500% for 300 meV.
- Published
- 2020
- Full Text
- View/download PDF
47. Active-sterile neutrino oscillations in low-reheating scenarios
- Author
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De Salas, P.F., Gariazzo, S., Pastor, Sergio, Fernández Navarro, Mario, De Salas, P.F., Gariazzo, S., Pastor, Sergio, and Fernández Navarro, Mario
- Published
- 2020
48. Constraining power of open likelihoods, made prior-independent
- Author
-
European Commission, SCOAP, Gariazzo, S., European Commission, SCOAP, and Gariazzo, S.
- Abstract
One of the most criticized features of Bayesian statistics is the fact that credible intervals, especially when open likelihoods are involved, may strongly depend on the prior shape and range. Many analyses involving open likelihoods are affected by the eternal dilemma of choosing between linear and logarithmic prior, and in particular in the latter case the situation is worsened by the dependence on the prior range under consideration. In this letter, we revive a simple method to obtain constraints that depend neither on the prior shape nor range and, using the tools of Bayesian model comparison, extend it to overcome the possible dependence of the bounds on the choice of free parameters in the numerical analysis. An application to the case of cosmological bounds on the sum of the neutrino masses is discussed as an example.
- Published
- 2020
49. Neutrino masses, states and interactions: Session summary
- Author
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Gariazzo S., Sisti M., Gariazzo, S, and Sisti, M
- Subjects
Neutrino oscillation ,Neutrino ma ,Double beta decay - Abstract
In these proceedings we present a brief summary of the parallel Session IV, “Neutrino masses, states and interactions”, part of the Neutrino Oscillation Workshop 2018∗. Topics of the session included the current status of some experimental searches for the neutrino absolute mass scale, a resume of recent results and developments in neutrinoless double beta decay, the situation of the search for a light sterile neutrino with a mass around 1 eV, a phenomenological summary on neutrino electromagnetic properties and a discussion about theoretical models for neutrino masses and mixings.
- Published
- 2018
50. Neutrino clustering in the Milky Way and beyond
- Author
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Mertsch, P., primary, Parimbelli, G., additional, de Salas, P.F., additional, Gariazzo, S., additional, Lesgourgues, J., additional, and Pastor, S., additional
- Published
- 2020
- Full Text
- View/download PDF
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