ESSnuSB collaboration
Autor: | Alekou, A., Baussan, E., Blaskovic Kraljevic, N., Blennow, M., Bogomilov, M., Bouquerel, E., Burgman, A., Carlile, C. J., Cederkall, J., Christiansen, P., Collins, M., Cristaldo Morales, E., Alessi, L. D., Danared, H., André, J. P. A. M., Delahaye, J. P., Dracos, M., Efthymiopoulos, I., Ekelöf, T., Eshraqi, M., Fanourakis, G., Fernandez-Martinez, E., Folsom, B., Ghosh, M., Gokbulut, G., Halić, L., Kayis Topaksu, A., Kliček, B., Krhač, K., Lindroos, M., Mezzetto, M., Oglakci, M., Ohlsson, T., Olvegård, M., Ota, T., Park, J., Petkov, G., Poussot, P., Rosauro-Alcaraz, S., Stavropoulos, G., Stipčević, M., Terranova, F., Thomas, J., Tolba, T., Tsenov, R., Vankova-Kirilova, G., Vassilopoulos, N., Wildner, E., jacques wurtz, Zormpa, O., Zou, Y. |
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Přispěvatelé: | HEP, INSPIRE, Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg (UNISTRA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), ESSnuSB, European Organization for Nuclear Research (CERN) |
Jazyk: | chorvatština |
Rok vydání: | 2021 |
Předmět: |
Physics - Instrumentation and Detectors
far detector QC770-798 hierarchy Astrophysics High Energy Physics - Experiment Subatomär fysik High Energy Physics - Experiment (hep-ex) neutrino High Energy Physics - Phenomenology (hep-ph) Subatomic Physics [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] neutrino: flux: calculated Detectors and Experimental Techniques physics.ins-det ComputingMilieux_MISCELLANEOUS Physics hep-ph Instrumentation and Detectors (physics.ins-det) essnusb cp violation QB460-466 High Energy Physics - Phenomenology neutrino: detector CP violation proposed experiment numerical calculations: Monte Carlo Particle Physics - Experiment performance [PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex] neutrino: mass difference FOS: Physical sciences Nuclear and particle physics. Atomic energy. Radioactivity ESSnuSB CP: violation conservation law mixing calculated flavor: 3 [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] Particle Physics - Phenomenology flavor hep-ex background sensitivity neutrino: mixing angle flux [PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph] [PHYS.PHYS.PHYS-INS-DET] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] atmosphere neutrino: oscillation neutrino: mixing |
Zdroj: | European physical journal C : particles and fields HAL European Physical Journal INSPIRE-HEP Eur.Phys.J.C Eur.Phys.J.C, 2021, 81 (12), pp.1130. ⟨10.1140/epjc/s10052-021-09845-8⟩ European Physical Journal C: Particles and Fields, Vol 81, Iss 12, Pp 1-12 (2021) |
DOI: | 10.1140/epjc/s10052-021-09845-8⟩ |
Popis: | In this paper, we present the physics performance of the ESSnuSB experiment in the standard three flavor scenario using the updated neutrino flux calculated specifically for the ESSnuSB configuration and updated migration matrices for the far detector. Taking conservative systematic uncertainties corresponding to a normalization error of $5\%$ for signal and $10\%$ for background, we find that there is $10\sigma$ $(13\sigma)$ CP violation discovery sensitivity for the baseline option of 540 km (360 km) at $\delta_{\rm CP} = \pm 90^\circ$. The corresponding fraction of $\delta_{\rm CP}$ for which CP violation can be discovered at more than $5 \sigma$ is $70\%$. Regarding CP precision measurements, the $1\sigma$ error associated with $\delta_{\rm CP} = 0^\circ$ is around $5^\circ$ and with $\delta_{\rm CP} = -90^\circ$ is around $14^\circ$ $(7^\circ)$ for the baseline option of 540 km (360 km). For hierarchy sensitivity, one can have $3\sigma$ sensitivity for 540 km baseline except $\delta_{\rm CP} = \pm 90^\circ$ and $5\sigma$ sensitivity for 360 km baseline for all values of $\delta_{\rm CP}$. The octant of $\theta_{23}$ can be determined at $3 \sigma$ for the values of: $\theta_{23} > 51^\circ$ ($\theta_{23} < 42^\circ$ and $\theta_{23} > 49^\circ$) for baseline of 540 km (360 km). Regarding measurement precision of the atmospheric mixing parameters, the allowed values at $3 \sigma$ are: $40^\circ < \theta_{23} < 52^\circ$ ($42^\circ < \theta_{23} < 51.5^\circ$) and $2.485 \times 10^{-3}$ eV$^2 < \Delta m^2_{31} < 2.545 \times 10^{-3}$ eV$^2$ ($2.49 \times 10^{-3}$ eV$^2 < \Delta m^2_{31} < 2.54 \times 10^{-3}$ eV$^2$) for the baseline of 540 km (360 km). Comment: 13 pages, 8 figures, 3 tables. Changes: Text updated, this is a published version |
Databáze: | OpenAIRE |
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