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Updated physics performance of the ESSnuSB experiment
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 co...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2021
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epjc/s10052-021-09845-8 http://cds.cern.ch/record/2776281 |
_version_ | 1780971613512007680 |
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author | 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. D'Alessi, L. Danared, H. de 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. Wurtz, J. Zormpa, O. Zou, Y. |
author_facet | 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. D'Alessi, L. Danared, H. de 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. Wurtz, J. Zormpa, O. Zou, Y. |
author_sort | Alekou, A. |
collection | CERN |
description | 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 _\mathrm{CP} = \pm 90^\circ $. The corresponding fraction of $\delta _\mathrm{CP}$ 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 _\mathrm{CP} = 0^\circ $ is around $5^\circ $ and with $\delta _\mathrm{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 _\mathrm{CP} = \pm 90^\circ $ and $5\sigma $ sensitivity for 360 km baseline for all values of $\delta _\mathrm{CP}$. 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$^2< \varDelta m^2_{31} < 2.545 \times 10^{-3}$ eV$^2$ ($2.49 \times 10^{-3}$ eV$^2< \varDelta m^2_{31} < 2.54 \times 10^{-3}$ eV$^2$) for the baseline of 540 km (360 km). |
id | cern-2776281 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2021 |
record_format | invenio |
spelling | cern-27762812023-08-25T02:59:02Zdoi:10.1140/epjc/s10052-021-09845-8http://cds.cern.ch/record/2776281engAlekou, 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. D'Alessi, L.Danared, H.de 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.Wurtz, J.Zormpa, O.Zou, Y.Updated physics performance of the ESSnuSB experimentphysics.ins-detDetectors and Experimental Techniqueshep-phParticle Physics - Phenomenologyhep-exParticle Physics - ExperimentIn 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 _\mathrm{CP} = \pm 90^\circ $. The corresponding fraction of $\delta _\mathrm{CP}$ 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 _\mathrm{CP} = 0^\circ $ is around $5^\circ $ and with $\delta _\mathrm{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 _\mathrm{CP} = \pm 90^\circ $ and $5\sigma $ sensitivity for 360 km baseline for all values of $\delta _\mathrm{CP}$. 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$^2< \varDelta m^2_{31} < 2.545 \times 10^{-3}$ eV$^2$ ($2.49 \times 10^{-3}$ eV$^2< \varDelta m^2_{31} < 2.54 \times 10^{-3}$ eV$^2$) for the baseline of 540 km (360 km).n 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% 5% for signal and 10% 10% for background, we find that there is 10𝜎 10σ (13𝜎) (13σ) CP violation discovery sensitivity for the baseline option of 540 km (360 km) at 𝛿 CP =± 90 ∘ δCP=±90∘. The corresponding fraction of 𝛿 CP δCP for which CP violation can be discovered at more than 5𝜎 5σ is 70% 70%. Regarding CP precision measurements, the 1𝜎 1σ error associated with 𝛿 CP = 0 ∘ δCP=0∘ is around 5 ∘ 5∘ and with 𝛿 CP =− 90 ∘ δCP=−90∘ is around 14 ∘ 14∘ ( 7 ∘ ) (7∘) for the baseline option of 540 km (360 km). For hierarchy sensitivity, one can have 3𝜎 3σ sensitivity for 540 km baseline except 𝛿 CP =± 90 ∘ δCP=±90∘ and 5𝜎 5σ sensitivity for 360 km baseline for all values of 𝛿 CP δCP. The octant of 𝜃 23 θ23 can be determined at 3𝜎 3σ for the values of: 𝜃 23 > 51 ∘ θ23>51∘ ( 𝜃 23 < 42 ∘ θ23<42∘ and 𝜃 23 > 49 ∘ θ23>49∘) for baseline of 540 km (360 km). Regarding measurement precision of the atmospheric mixing parameters, the allowed values at 3𝜎 3σ are: 40 ∘ < 𝜃 23 < 52 ∘ 40∘<θ23<52∘ ( 42 ∘ < 𝜃 23 < 51.5 ∘ 42∘<θ23<51.5∘) and 2.485× 10 −3 2.485×10−3 eV 2 <𝛥 𝑚 2 31 <2.545× 10 −3 2<Δm312<2.545×10−3 eV 2 2 ( 2.49× 10 −3 2.49×10−3 eV 2 <𝛥 𝑚 2 31 <2.54× 10 −3 2<Δm312<2.54×10−3 eV 2 2) for the baseline of 540 km (360 km).`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).arXiv:2107.07585oai:cds.cern.ch:27762812021-06-25 |
spellingShingle | physics.ins-det Detectors and Experimental Techniques hep-ph Particle Physics - Phenomenology hep-ex Particle Physics - Experiment 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. D'Alessi, L. Danared, H. de 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. Wurtz, J. Zormpa, O. Zou, Y. Updated physics performance of the ESSnuSB experiment |
title | Updated physics performance of the ESSnuSB experiment |
title_full | Updated physics performance of the ESSnuSB experiment |
title_fullStr | Updated physics performance of the ESSnuSB experiment |
title_full_unstemmed | Updated physics performance of the ESSnuSB experiment |
title_short | Updated physics performance of the ESSnuSB experiment |
title_sort | updated physics performance of the essnusb experiment |
topic | physics.ins-det Detectors and Experimental Techniques hep-ph Particle Physics - Phenomenology hep-ex Particle Physics - Experiment |
url | https://dx.doi.org/10.1140/epjc/s10052-021-09845-8 http://cds.cern.ch/record/2776281 |
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