Nicolò Macaluso
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
The proton boron-11 fusion reaction is gaining interest as aneutronic alternative to conventional fusion approaches, due to its characteristic to produce three alpha particles without neutron emission. This feature makes it attractive for clean energy production with reduced radiological impact.
In this context, an experimental campaign was conduced at the PALS facility in 2024 to investigate alpha particle production from boron-enriched targets irradiated with a high-intensity laser. The study employed a mixed setup combining both “in-target” and “pitcher-catcher” configurations. The main laser pulse interacts with a primary target, initiating both in-target fusion reaction and the emission of energetic particles (mainly protons). These particles then strike a secondary thick target composed of natural boron, where further p($^{11}$B,α)2α ructions occur in the pitcher-catcher configuration.
Various diagnostics were employed during the experiment, including Time of Flight (TOF) systems for real-time monitoring, Thomson Parabola (TP) spectrometers for ion characterization, and CR39 nuclear track detectors for particle identification. This work focuses on the fusion reactions occurring in the secondary target. Alpha particles emitted from the boron target were detected using CR39 detectors positioned in front of the target shielded with aluminum filters of varying thickness to suppress low-energy background contributions. Preliminary analysis of the CR39 detectors indicates an estimated alpha fluence of about 10$^5$ α/cm$^2$, meaning a yield of 10$^6$ α/str.
A key aspect of the experiment was the successful activation of the natural boron target (secondary) by the ion beam produced via the ablation and the backward acceleration of the protons from the primary target. Activation was quantified using an HPGe detector, leading to an estimate of approximately 10$^7$ proton boron-11 fusion reactions occurring inside the secondary target per laser shot.
To support and interpret the experimental results, Monte Carlo simulations were carried out. A first simulations, incorporating the experimentally measured proton and carbon spectra from the TP diagnostic, evaluated the impact of backscattered ions (protons and carbons) on CR39 signals. Another simulation then was carried out to study the alpha emission from the thick secondary natural boron target and compare it with CR39 measurements.
In summary, this study combines various experimental diagnostics and numerical modeling to validate the alpha yield measurements, with particular attention to CR39 detectors, which are especially challenging to interpret.
Nicolò Macaluso
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
A. D. Pappalardo
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
A. M. Raso
(Dipartimento di Ingegneria Industriale, Università di Roma “Tor Vergata)
A. Picciotto
(Micro Nano Facility and Custom Radiation Sensors, Sensors and Devices Centre, Fondazione Bruno Kessler)
A. Scandurra
(Dipartimento di Fisica e Astronomia, Università̀ degli Studi di Catania)
A. Trifirò
(Dip. MIFT - Università di Messina and INFN section of Catania)
B. Grau
(Dipartimento di Ingegneria Industriale, Università di Roma “Tor Vergata)
C. Altana
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
C. Ciampi
(Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF–CNRS/IN2P3, Boulevard Henri Becquerel)
C. Verona
(Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tor Vergata)
D. Bortot
(Politecnico di Milano, Dipartimento di Energia and INFN - sezione di Milano,)
D. Ettel
(FZU - Institute of Physics, Czech Academy of Sciences Na Slovance)
D. Margarone
(ELI Beamlines Facility, The Extreme Light Infrastructure ERIC)
D. Santonocito
(Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare (LNS-INFN))
E. Domenicone
(National Institute for Nuclear Physics (INFN) and Physics Department Milano-Bicocca)
E. Pagano
(Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare (LNS-INFN))
F. Consoli
(ENEA - Dipartimento Fusione e Tecnologie per la Sicurezza Nucleare, CR Frascati)
Dr
Farmesk Abubaker
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
G. A. P. Cirrone
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
G. Cantone
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
G. Messina
(Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare (LNS-INFN))
G. Morello
(Center for Biomolecular Nanotechnologies @UNILE, Istituto Italiano di Tecnologia)
G. Petringa
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
G. Rapisarda
(Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare (LNS-INFN))
J. Krasa
(INFN - sezione di Milano)
L. Giuffrida
(ELI Beamlines Facility, The Extreme Light Infrastructure ERIC)
L. Guardo
(Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare (LNS-INFN), Catania 95125, Italy)
L. Juha
(FZU - Institute of Physics, Czech Academy of Sciences Na Slovance)
L. Malferrari
(CNR IMM – Institute for Microelectronics and Microsystems - Unit of Lecce)
M. Alonzo
(Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tor Vergata)
M. Cervenak
(Institute of Plasma Physics, Czech Academy of Sciences)
M. Cipriani
(Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tor Vergata)
M. Krupka
(FZU - Institute of Physics, Czech Academy of Sciences Na Slovance)
M. Krus
(nstitute of Plasma Physics, Czech Academy of Sciences)
M. Rosinski
(Institute of Plasma Physics and Laser Microfusion,)
M. Scisciò
(ENEA - Dipartimento Fusione e Tecnologie per la Sicurezza Nucleare, CR Frascati)
Marco La Cognata
(Istituto Nazionale di Fisica Nucleare)
P. Devi
(FZU - Institute of Physics, Czech Academy of Sciences)
P. Gajdos
(Institute of Plasma Physics, Czech Academy of Sciences Za Slovankou)
P. Tchórz
(Institute of Plasma Physics and Laser Microfusion)
R. Catalano
(Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare (LNS-INFN))
R. Dudzak
(Institute of Plasma Physics, Czech Academy of Sciences Za Slovankou)
R. Rinaldi
(Department of Mathematics and Physics “Ennio De Giorgi”, University of Salento)
S. Agarwal
(FZU - Institute of Physics, Czech Academy of Sciences)
S. Arjmand
(Istituto Nazionale di Fisica Nucleare-Laboratori Nazionali del Sud, Catania (IT))
S. Mirabella
(Dipartimento di Fisica e Astronomia, Università̀ degli Studi di Catania)
S. Singh
(Institute of Plasma Physics, Czech Academy of Sciences)
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