19-21 noviembre 2024
Madrid
Europe/Madrid timezone

Status and perspectives of (alpha,n) reactions measurements at CNA HiSPANoS

19 nov. 2024 16:37
7m
Red Temática de Física Nuclear (FNUC) Red FNUC (Red Temática de Física Nuclear)

Ponente

Carlos Guerrero (Universidad de Sevilla)

Descripción

Neutron emitted in nuclear reactions following the absorption of alpha particles play a key role in several fields of research: acting as neutron source in the s-process, affecting the production of elements in the r-process occurring in the neutron driven winds of core-collapse supernova, inducing background signals in underground dark matter search experiments, or being a proxy for active interrogation of nuclear materials. Accordingly, there is a renewed interest in measuring the yields and energy spectra of (alpha,n) reactions on many isotopes (see. Ref. [1] for a recent overview of the scientific cases and a summary of the reactions of interest in the mentioned fields of research). In this context, the Spanish experimental nuclear physics community has established the MANY (Measurements of Alpha-N Yields) Collaboration to measure (alpha,n) reactions at two different accelerator facilities (CNA HiSPANoS [2,3] and CMAM [4]) using three complementary detectors for assessing the corresponding neutron yields (miniBELEN [5] and GARY [6]) and energy spectra (MONSTER [7]).

The CNA HiSPANoS facility is driven by a 3 MV tandem accelerator delivering both continuous and pulsed (2% duty cycle) beams of proton/deuteron up to 6 MeV and alphas up to 9 MeV. The current source of alphas is a NEC-ALPHATROSS model delivering a maximum current of only 2 uA, and the pulsing systems is only designed and optimized for protons and deuterons, hence performing poorly for alpha beams. This configuration is well suited for activation and neutron counting experiments with miniBELEN, which shall start in early 2025, and the results from preliminary measurements on 27Al(alpha,n) by ToF using the pulsed beam and a single MONSTER neutron detector module are promising. However, the limitations in beam current and pulsing performance have called for a major upgrade. First, a more versatile buncher system is currently being designed by NEC and <2 ns bunches of alpha particles will be available by Fall 2025. Furthermore, the necessary funds have been secured to purchase and install a NEC-TORVIS ion source capable of delivering alpha beam currents one order of magnitude higher, i.e. 20 uA.

[1] D. Cano-Ott et al., arXiv:2405.07952 (2024)
[2] J. Gómez-Camacho et al., Eur. Phys. J. Plus, 136:273 (2021)
[3] M.A. Millán-Callado et al., Rad. Phys. and Chem. 217 (2024) 111464
[4] A. Redondo-Cubero et al., Eur. Phys. J. Plus 136:175 (2021)
[5] N. Mont-Geli et al., Eur. Phys. J. Web of Conf., 284 (2023) 06004
[6] L.M. Fraile et al., “Measurement of Al(,n) P thick-target yields and total Al(α,n) yields by activation”, IAEA 2nd TM on (,n) Reaction Nuclear Data Evaluations and Data Needs (2023)
[7] T. Martínez et al., Nucl. Data Sheets 120 (2014) 78-80
[8] G. J. H. Jacobs and H. Liskien, Annals of Nucl. Energy 10, 541 (1983)

Abstract

Neutron emitted in nuclear reactions following the absorption of alpha particles play a key role in several fields of research: acting as neutron source in the s-process, affecting the production of elements in the r-process occurring in the neutron driven winds of core-collapse supernova, inducing background signals in underground dark matter search experiments, or being a proxy for active interrogation of nuclear materials. Accordingly, there is a renewed interest in measuring the yields and energy spectra of (alpha,n) reactions on many isotopes (see. Ref. [1] for a recent overview of the scientific cases and a summary of the reactions of interest in the mentioned fields of research). In this context, the Spanish experimental nuclear physics community has established the MANY (Measurements of Alpha-N Yields) Collaboration to measure (alpha,n) reactions at two different accelerator facilities (CNA HiSPANoS [2,3] and CMAM [4]) using three complementary detectors for assessing the corresponding neutron yields (miniBELEN [5] and GARY [6]) and energy spectra (MONSTER [7]).

The CNA HiSPANoS facility is driven by a 3 MV tandem accelerator delivering both continuous and pulsed (2% duty cycle) beams of proton/deuteron up to 6 MeV and alphas up to 9 MeV. The current source of alphas is a NEC-ALPHATROSS model delivering a maximum current of only 2 uA, and the pulsing systems is only designed and optimized for protons and deuterons, hence performing poorly for alpha beams. This configuration is well suited for activation and neutron counting experiments with miniBELEN, which shall start in early 2025, and the results from preliminary measurements on 27Al(alpha,n) by ToF using the pulsed beam and a single MONSTER neutron detector module are promising. However, the limitations in beam current and pulsing performance have called for a major upgrade. First, a more versatile buncher system is currently being designed by NEC and <2 ns bunches of alpha particles will be available by Fall 2025. Furthermore, the necessary funds have been secured to purchase and install a NEC-TORVIS ion source capable of delivering alpha beam currents one order of magnitude higher, i.e. 20 uA.

[1] D. Cano-Ott et al., arXiv:2405.07952 (2024)
[2] J. Gómez-Camacho et al., Eur. Phys. J. Plus, 136:273 (2021)
[3] M.A. Millán-Callado et al., Rad. Phys. and Chem. 217 (2024) 111464
[4] A. Redondo-Cubero et al., Eur. Phys. J. Plus 136:175 (2021)
[5] N. Mont-Geli et al., Eur. Phys. J. Web of Conf., 284 (2023) 06004
[6] L.M. Fraile et al., “Measurement of Al(,n) P thick-target yields and total Al(α,n) yields by activation”, IAEA 2nd TM on (,n) Reaction Nuclear Data Evaluations and Data Needs (2023)
[7] T. Martínez et al., Nucl. Data Sheets 120 (2014) 78-80
[8] G. J. H. Jacobs and H. Liskien, Annals of Nucl. Energy 10, 541 (1983)

Autores primarios

Carlos Guerrero (Universidad de Sevilla) Victor Alcayne Aicua (CIEMAT (Spain)) Alejandro Algora (IFIC (CSIC-Univ. Valencia)) Sr. Gabriel Auñón (Universidad de Sevilla) Diana Bachiller-Perea (IJCLab (CNRS, Université de Paris, Université Paris-Saclay)) Javier Balibrea Correa (Instituto de física corpuscular IFIC) Jaime Benito García (Grupo de Fisíca Nuclear, Facultad de Ciencias Físicas, Universidad Complutense de Madrid- CEI Moncloa, E-28040 Madrid, Spain) Maria Jose Garcia Borge (Instituto de Estructura de la Materia) Dr. José Antonio Briz Monago (Universidad Complutense de Madrid) Francisco Calvino (Universitat Politecnica de Catalunya) Daniel Cano Ott (CIEMAT) Guillem Cortes Rossell (Universitat Politecnica de Catalunya. Dep. Física i Enginyeria Nuclear) Alfredo De Blas Del Hoyo (UPC - Universitat Politècnica de Catalunya) Cesar Domingo-Pardo (IFIC (CSIC-University of Valencia)) Begoña Fernández (Centro Naciona de Aceleradores) Luis Mario Fraile (Universidad Complutense de Madrid) Roger Garcia Sanchez (UPC - Universitat Politècnica de Catalunya) Dr. Gastón García (Universidad Autónoma de Madrid (UAM)) Dr. Enrique González-Romero (CIEMAT) Jorge Lerendegui Marco (Instituto de Física Corpuscular) Sr. José Llanes-Gamonoso (CIEMAT) Marcos Llanos Expósito (UCM) Trinitario Martínez Pérez (CIEMAT) Emilio Mendoza (CIEMAT) Nil Mont i Geli (Universitat Politècnica de Catalunya) Sr. Javier Murias (UCM) Enrique Nacher (Instituto de Física Corpuscular - CSIC) Sr. Jorge Nacher Arandiga (IFIC) Dr. Sonja Orrigo (IFIC (CSIC-UV)) Max Pallàs Solís (Universitat Politècnica de Catalunya (UPC)) Angel Perea Martinez (IEM/CSIC) Alberto Pérez de Rada Fiol (CIEMAT) Vicente Pesudo Fortes (CIEMAT / LSC) Julio Plaza del Olmo (CIEMAT) Víctor Sánchez-Tembleque Verbo (Grupo de FIsica Nuclear) Roberto Santorelli (Ciemat) Jose L. Tain (Instituto de Fisica Corpuscular) Ariel Tarifeño-Saldivia (Instituto de Fisica Corpuscular (CSIC-UV)) Olof Tengblad (IEM -CSIC) Jose Udias (Universidad Complutense de Madrid) David Villamarín Fernández (CIEMAT) Sílvia Viñals Onsès (CSIC - IEM)

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