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1

Ning, Xiaochuan, Tianyi Liang, Dong Wu, et al. "Laser-Driven Proton-Boron Fusions: Influences of the Boron State." Laser and Particle Beams 2022 (September 26, 2022): 1–7. http://dx.doi.org/10.1155/2022/9868807.

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The proton-boron (p 11 B) reaction is regarded as the holy grail of advanced fusion fuels, where the primary reaction produces 3 energetic α particles. However, due to the high nuclear bounding energy and bremsstrahlung energy losses, energy gain from the p 11 B fusion is hard to achieve in thermal fusion conditions. Owing to advances in intense laser technology, the p 11 B fusion has drawn renewed attention by using an intense laser-accelerated proton beam to impact a boron-11 target. As one of the most influential works in this field, Labaune et al. first experimentally found that states of
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2

Cartlidge, Edwin. "Proton–boron fusion passes milestone." Physics World 36, no. 4 (2023): 7. http://dx.doi.org/10.1088/2058-7058/36/04/08.

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3

Batani, K. "Perspectives on research on laser driven proton-boron fusion and applications." Journal of Instrumentation 18, no. 09 (2023): C09012. http://dx.doi.org/10.1088/1748-0221/18/09/c09012.

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Abstract Recent experiments with high-intensity lasers have shown record production of α-particles by irradiating boron-hydrogen targets. This opened the way to completely new studies on proton-boron fusion with multiple goals: i) studies related to nuclear fusion. The proton-boron fusion reaction produces 3 α-particles and releases a large energy. It is considered an interesting alternative to deuterium-tritium fusion because it produces no neutrons, therefore no activation and radioactive wastes. ii) generation of novel laser-driven α-particle sources. Laser-driven α-particle sources are pro
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4

Kurmanova, A., G. Petringa, R. Catalano, and G. A. P. Cirrone. "Design of a compact Thomson Parabola Spectrometer for diagnostics of proton-boron fusion reaction products initiated by laser." Journal of Instrumentation 18, no. 06 (2023): C06027. http://dx.doi.org/10.1088/1748-0221/18/06/c06027.

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Abstract The proton-boron aneutronic fusion reaction has numerous potential applications varying from controlled nuclear fusion reactor to broad-energy spectrum α-particle source, as well as uses in medicine, where it can serve as a source for radioisotope production, or directly in proton boron capture therapy. However, proton-boron fusion reaction and its by-products should be investigated extensively to provide a stable and controlled secondary ion source. In order to monitor the multi-ion beam emitted and accelerated from the target surface after interaction with laser pulses, a new Thomso
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5

Schollmeier, Marius S., Vahe Shirvanyan, Christie Capper, et al. "Investigation of Proton Beam-Driven Fusion Reactions Generated by an Ultra-Short Petawatt-Scale Laser Pulse." Laser and Particle Beams 2022 (October 13, 2022): 1–13. http://dx.doi.org/10.1155/2022/2404263.

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We present results from a pitcher-catcher experiment utilizing a proton beam generated with nanostructured targets at a petawatt-class, short-pulse laser facility to induce proton-boron fusion reactions in a secondary target. A 45-fs laser pulse with either 400 nm wavelength and 7 J energy, or 800 nm and 14 J, and an intensity of up to 5 × 1021 W/cm2 was used to irradiate either thin foil targets or near-solid density, nanostructured targets made of boron nitride (BN) nanotubes. In particular, for 800 nm wavelength irradiation, a BN nanotube target created a proton beam with about five times h
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6

Akkoyun, Serkan. "Estimation of proton-boron reaction cross-sections by neural networks." International Conference on Applied Engineering and Natural Sciences 1, no. 1 (2023): 71–73. http://dx.doi.org/10.59287/icaens.967.

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The proton-boron fusion reaction is one of the interesting reactions in nuclear energy production. The fact that neutrons and radioactive products do not come out as a result of the reaction makes these reactions special. However, the realization of this reaction is very difficult due to the low reactivity of the plasma and high radiation losses at temperatures achievable in today's fusion devices. Therefore, it is important to determine the cross-sections of these reactions. In our study, we obtained the cross-sections of proton-boron fusion reactions using the machine learning methods after
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7

DONG 董, Jiaqi 家齐, Wei 伟. CHEN 陈, Zhongyong 忠勇 CHEN 陈, et al. "Thermal proton-boron fusion on spherical torus." Plasma Science and Technology 27, no. 2 (2025): 020101. https://doi.org/10.1088/2058-6272/adb36a.

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8

Gruenwald, Johannes, and Leonel Morejon. "Numerical studies of a layered lithium-boron target for laser-driven aneutronic fusion reactions." Journal of Technological and Space Plasmas 4, no. 1 (2023): 123–32. http://dx.doi.org/10.31281/jtsp.v4i1.27.

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This paper explores a novel target design for laser-driven, aneutronic, proton-boron and proton-lithium fusion reactions consisting of a stack of boron and lithium foils. In contrast to a homogeneous target, this multi-layer setup provides additional fusion channels in the different materials. The composition of the layers is chosen in descending order of the fusion reactions' thresholds, facilitating the fusion of protons that penetrate further into the material despite their energy losses due to electronic and nuclear stopping power. We employ a combination of Fluka simulations and additiona
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9

Martinez-Val, J. M., S. Eliezer, M. Piera, and G. Velarde. "Fusion burning waves in proton-boron-11 plasmas." Physics Letters A 216, no. 1-5 (1996): 142–52. http://dx.doi.org/10.1016/0375-9601(96)00252-6.

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10

Baccou, C., S. Depierreux, V. Yahia, et al. "New scheme to produce aneutronic fusion reactions by laser-accelerated ions." Laser and Particle Beams 33, no. 1 (2015): 117–22. http://dx.doi.org/10.1017/s0263034615000178.

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AbstractThe development of high-intensity lasers has opened the field of nuclear reactions initiated by laser-accelerated particles. One possible application is the production of aneutronic fusion reactions for clean fusion energy production. We propose an innovative scheme based on the use of two targets and present the first results obtained with the ELFIE facility (at the LULI Laboratory) for the proton–boron-11 (p–11B) fusion reaction. A proton beam, accelerated by the Target Normal Sheat Acceleration mechanism using a short laser pulse (12 J, 350 fs, 1.056 µm, 1019 W cm−2), is sent onto a
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11

Turcu, I. C. E., D. Margarone, L. Giuffrida, et al. "Borane (B m H n ), Hydrogen rich, Proton Boron fusion fuel materials for high yield laser-driven Alpha sources." Journal of Instrumentation 19, no. 03 (2024): C03065. http://dx.doi.org/10.1088/1748-0221/19/03/c03065.

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Abstract We propose for the first time, a new fuel-material for laser-driven Proton Boron (P-B) fusion nuclear reactions. We propose, Hydrogen rich, Borane (B m H n ) materials as fusion fuel as compared to Boron Nitride (BN) presently used. We estimate more than 10-fold increase in the yield of nuclear fusion reactions, and Alpha-prticle flux, when, for example Ammonia Borane (BNH6) laser-target material will be used compared to the state of the art normalized flux ∼108 Alphas/sr/J from BN targets. BNH6 contains ∼1000× higher concentration of Hydrogen compared to BN. We report the manufacture
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12

Cammarata, F. P., F. Torrisi, A. M. Pavone, et al. "A novel boron-conjugated SRC inhibitor for Proton Boron Capture Therapy in glioblastoma treatment." Journal of Instrumentation 19, no. 04 (2024): C04051. http://dx.doi.org/10.1088/1748-0221/19/04/c04051.

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Abstract The ability of protons to deliver the maximum dose at the tumor region can work synergistically with boron atoms to emit alpha particles, enhancing therapy effects with less damage to healthy tissue. Protons and boron nuclear fusion reaction is the principle for the so-called Proton Boron Capture Therapy, that can contribute to high therapy efficiency by using smaller flux than conventional proton therapy, especially for radioresistant brain tumors such as glioblastoma. Glioblastoma is the most infiltrating and aggressive tumor of the brain with a very low life expectancy, ranging fro
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13

Kurilenkov, Yu K., V. P. Tarakanov, A. V. Oginov, S. Yu Gus’kov, and I. S. Samoylov. "Oscillating Plasmas for Proton- Boron Fusion in Miniature Vacuum Discharge." Laser and Particle Beams 2023 (March 4, 2023): 1–10. http://dx.doi.org/10.1155/2023/9563197.

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Earlier, the experiments on the aneutronic proton-boron (pB) fusion in a miniature nanosecond vacuum discharge (NVD) with oscillatory plasma confinement and correspondent α particles yield were presented. In this work, we consider some specific features of oscillatory confinement as a relatively new type of plasma confinement for fusion. Particle-in-cell (PiC) simulations of pB fusion processes have shown that the plasma in NVD, and especially on the discharge axis, is in a state close to a quasineutral one, which is rather different from the conditions in the well-known scheme of periodically
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14

Margarone, Daniele, Julien Bonvalet, Lorenzo Giuffrida, et al. "In-Target Proton–Boron Nuclear Fusion Using a PW-Class Laser." Applied Sciences 12, no. 3 (2022): 1444. http://dx.doi.org/10.3390/app12031444.

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Nuclear reactions between protons and boron-11 nuclei (p–B fusion) that were used to yield energetic α-particles were initiated in a plasma that was generated by the interaction between a PW-class laser operating at relativistic intensities (~3 × 1019 W/cm2) and a 0.2-mm thick boron nitride (BN) target. A high p–B fusion reaction rate and hence, a large α-particle flux was generated and measured, thanks to a proton stream accelerated at the target’s front surface. This was the first proof of principle experiment to demonstrate the efficient generation of α-particles (~1010/sr) through p–B fusi
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15

Moustaizis, S., C. Daponta, S. Eliezer, et al. "Alpha heating and avalanche effect simulations for low density proton-boron fusion plasma." Journal of Instrumentation 19, no. 01 (2024): C01015. http://dx.doi.org/10.1088/1748-0221/19/01/c01015.

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Abstract The initial interest in p-11B fusion, which produces three (3) alpha particles with total energy of 8.7 MeV, was regained the last few years, due to the important experimental measurements on alpha particle production and theoretical and numerical investigations. The re-evaluation of proton-boron fusion, as an important vector for “aneutronic” energy production, is based on the consideration of the “chain reactions alpha heating effect and the related avalanche effect”, as the important process, for the increase of the fusion species (p, 11B) temperatures, to temperatures correspondin
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16

Dimitrijević, Milan S., Magdalena D. Christova, and Sylvie Sahal-Bréchot. "Stark Broadening of N VI Spectral Lines." Universe 9, no. 12 (2023): 511. http://dx.doi.org/10.3390/universe9120511.

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Stark broadening parameters, line widths and shifts, for 15 N VI multiplets are calculated using semiclassical perturbation theory for temperatures from 50,000 K to 2,000,000 K, and perturber density of 1016 cm−3. As perturbers have been taken electrons, protons and He III ions (alpha particles), which are of interest particularly for white dwarfs. Moreover, B III, B IV, B V and B VI ions have been taken as well, due to their significance for proton-boron fusion investigations. An example of the importance of Stark broadening in comparison with thermal Doppler broadening in atmospheres of spec
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17

Hora, Heinrich, Shalom Eliezer, and Noaz Nissim. "Elimination of Secondary Neutrons from Laser Proton-Boron Fusion." Laser and Particle Beams 2021 (April 7, 2021): 1–3. http://dx.doi.org/10.1155/2021/9978899.

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For low carbon energy generation, a very large exchange of electricity generators is existentially vital within the next number of years by power stations preferably at considerably low cost than the present installations. When considering the million times higher nuclear energy per reaction than chemical, the usual hydrogen fusion with abundant boron fuel is used for environmentally clean electricity generators. Instead of usually needed ignition temperatures of hundreds of million degrees Celsius, it is possible to use nonthermal ignition pressures from now available CPA laser pulses. In thi
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18

Eliezer, Shalom, Heinrich Hora, Georg Korn, Noaz Nissim, and Josè Maria Martinez Val. "Avalanche proton-boron fusion based on elastic nuclear collisions." Physics of Plasmas 23, no. 5 (2016): 050704. http://dx.doi.org/10.1063/1.4950824.

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19

Qin, T. T., W. Luo, H. Y. Lan, and W. M. Wang. "Ultrafast probing of plasma ion temperature in proton–boron fusion by nuclear resonance fluorescence emission spectroscopy." Matter and Radiation at Extremes 7, no. 3 (2022): 035901. http://dx.doi.org/10.1063/5.0078961.

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Aneutronic fusion reactions such as proton–boron fusion could efficiently produce clean energy with quite low neutron doses. However, as a consequence, conventional neutron spectral methods for diagnosing plasma ion temperature would no longer work. Therefore, finding a way to probe the ion temperature in aneutronic fusion plasmas is a crucial task. Here, we present a method to realize ultrafast in situ probing of 11B ion temperature for proton–boron fusion by Doppler broadening of the nuclear resonance fluorescence (NRF) emission spectrum. The NRF emission is excited by a collimated, intense
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20

Yinghuai, Zhu, Xinglong Lin, Hongming Xie, Jianlin Li, Narayan S. Hosmane, and Yingjun Zhang. "The Current Status and Perspectives of Delivery Strategy for Boronbased Drugs." Current Medicinal Chemistry 26, no. 26 (2019): 5019–35. http://dx.doi.org/10.2174/0929867325666180904105212.

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Boron-containing compounds are essential micronutrients for animals and plants despite their low-level natural occurrence. They can strengthen the cell walls of the plants and they play important role in supporting bone health. However, surprisingly, boron-containing compounds are seldom found in pharmaceutical drugs. In fact, there are no inherent disadvantages reported so far in terms of the incorporation of boron into medicines. Indeed, drugs based on boron-containing compounds, such as tavaborole (marked name Kerydin) and bortezomib (trade name Velcade) have been investigated and they are
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21

Jamborová, Zuzana, Kateřina Pachnerová Brabcová, Anna Jelínek Michaelidesová, et al. "RADIATION DAMAGE TO DNA PLASMIDS IN THE PRESENCE OF BOROCAPTATES." Radiation Protection Dosimetry 198, no. 9-11 (2022): 532–36. http://dx.doi.org/10.1093/rpd/ncac094.

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Abstract Boron derivatives have great potential in cancer diagnostics and treatment. Borocaptates are used in boron neutron capture therapy and potentially in proton boron fusion therapy. This work examines modulation effects of two borocaptate compounds on radiation-induced DNA damage. Aqueous solutions of pBR322 plasmid containing increasing concentrations of borocaptates were irradiated with 60Co gamma rays or 30 MeV protons. Induction of single and double DNA strand breaks was investigated using agarose gel electrophoresis. In this model system, representing DNA without the intervention of
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22

Batani, Dimitri, Daniele Margarone, and Fabio Belloni. "Advances in the Study of Laser-Driven Proton-Boron Fusion." Laser and Particle Beams 2023 (June 13, 2023): 1–3. http://dx.doi.org/10.1155/2023/9824024.

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The topic of proton-boron fusion has recently attracted considerable interest in the scientific community, both for its future perspectives for energy production and for nearer-term possibilities to realize high-brightness α-particle sources. Very interesting experimental results have been obtained, in particular in laser-driven experiments but also using other experimental approaches. The goal of this special issue is to collect the most recent developments in experiments, theory, advanced targetry, diagnostics, and numerical simulation codes.
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23

Hegelich, B. M., L. Labun, O. Z. Labun, and T. A. Mehlhorn. "Photon and Neutron Production as In Situ Diagnostics of Proton-Boron Fusion." Laser and Particle Beams 2023 (May 8, 2023): 1–14. http://dx.doi.org/10.1155/2023/6924841.

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Short-pulse, ultrahigh-intensity lasers have opened new regimes for studying fusion plasmas and creating novel ultrashort ion beams and neutron sources. Diagnosing the plasma in these experiments is important for optimizing the fusion yield but difficult due to the picosecond time scales, 10 s of micron-cubed volumes, and high densities. We propose to use the yields of photons and neutrons produced by parallel reactions involving the same reactants to diagnose the plasma conditions and predict the yields of specific reactions of interest. In this work, we focus on verifying the yield of the hi
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De Angelis, Riccardo, Danilo Giulietti, Lucio Calcagnile та ін. "α particle space distribution from fusion reactions in Boron irradiated by mono-energetic protons". EPJ Web of Conferences 167 (2018): 05005. http://dx.doi.org/10.1051/epjconf/201816705005.

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This work presents results regarding the p + 11B → 3α + 8.7MeV aneutronic fusion reaction. We obtained such results by directing a 0.675 MeV proton beam from a Tandetron accelerator to a solid Boron sample, varying the incidence angle. Three different detectors were used to reveal the alpha particles emitted during the experiments. The evidence obtained leads us to propose an innovative scheme to investigate the yield of the aneutronic reaction when the proton beam is directed against a 11B laser induced plasma.
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25

LIU, Dong, Sue Lynn LEE, and Jong-Kwan WO*. "Evaluation of Proton-Boron Fusion-Enhanced Proton Therapy (PBFEPT) by Using a Simulation Method." New Physics: Sae Mulli 69, no. 2 (2019): 215–20. http://dx.doi.org/10.3938/npsm.69.215.

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26

Andreev, Stepan N., Yuri K. Kurilenkov, and Alexander V. Oginov. "Fully Electromagnetic Code KARAT Applied to the Problem of Aneutronic Proton–Boron Fusion." Mathematics 11, no. 18 (2023): 4009. http://dx.doi.org/10.3390/math11184009.

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In this paper, the full electromagnetic code KARAT is presented in detail, the scope of which is a computational experiment in applied problems of engineering electrodynamics. The basis of the physical model used is Maxwell’s equations together with boundary conditions for fields, as well as material equations linking currents with field strengths. The Particle in Cell (PiC) method for the kinetic description of plasma is implemented in the code. A unique feature of the code KARAT is the possibility of the self-consistent modeling of inelastic processes, in particular, nuclear reactions, at ea
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27

Hideghéty, Katalin, Rita Emilia Szabó, Róbert Polanek, Zoltán Szabó, Szilvia Brunner, and Tünde Tőkés. "New approaches in clinical application of laser-driven ionizing radiation." Proc. SPIE 10239, Medical Applications of Laser-Generated Beams of Particles IV: Review of Progress and Strategies for the Future 10239 (May 16, 2017): 102390A. https://doi.org/10.1117/12.2268300.

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The planned laser-driven ionizing beams (photon, very high energy electron, proton, carbon ion) at laser facilities have the unique property of ultra-high dose rate (>Gy/s^-10), short pulses, and at ELI-ALPS high repetition rate, carry the potential to develop novel laser-driven methods towards compact hospital-based clinical application. The enhanced flexibility in particle and energy selection, the high spatial and time resolution and extreme dose rate could be highly beneficial in radiotherapy. These approaches may increase significantly the therapeutic index over the currently available
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28

Eliezer, S., and J. M. Martínez-Val. "Proton–boron-11 fusion reactions induced by heat-detonation burning waves." Laser and Particle Beams 16, no. 4 (1998): 581–98. http://dx.doi.org/10.1017/s0263034600011411.

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Proton-boron-11 is the clean fusion reactionpar excellence, but it is very difficult to exploit it because of the very high ignition temperature of this reaction and its moderate fusion yield. In this paper, a proposal is made to induce these reactions by a heat-detonation wave that expands across a compressed target. The front of the wave has a double-layer structure, with a first front driven by electron heat conduction and a second front heated by α-particle energy deposition. Both fronts create a hot plasma where the stopping power is dominated by ions. The wave is originated by an ignitor
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29

Jung, Joo-Young, Do-Kun Yoon, Heui Chang Lee, Bo Lu, and Tae Suk Suh. "The investigation of physical conditions of boron uptake region in proton boron fusion therapy (PBFT)." AIP Advances 6, no. 9 (2016): 095119. http://dx.doi.org/10.1063/1.4963741.

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30

Yoon, Do-Kun, Naotaka Naganawa, Mitsuhiro Kimura, et al. "Application of proton boron fusion to proton therapy: Experimental verification to detect the alpha particles." Applied Physics Letters 115, no. 22 (2019): 223701. http://dx.doi.org/10.1063/1.5128953.

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31

Shin, Han-Back, Moo-Sub Kim, Sunmi Kim, et al. "Quantitative analysis of prompt gamma ray imaging during proton boron fusion therapy according to boron concentration." Oncotarget 9, no. 3 (2017): 3089–96. http://dx.doi.org/10.18632/oncotarget.23201.

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32

Mazzucconi, D., D. Vavassori, D. Dellasega, et al. "Proton boron fusion reaction: A novel experimental strategy for cross section investigation." Radiation Physics and Chemistry 204 (March 2023): 110727. http://dx.doi.org/10.1016/j.radphyschem.2022.110727.

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33

Bustreo, Chiara, and Roberto Cavazzana. "Newborn alpha particles from proton-boron fusion reactions in magnetically confined plasma." Joule 7, no. 4 (2023): 624–25. http://dx.doi.org/10.1016/j.joule.2023.03.022.

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34

Teng, Qiu-Xu, Guodong Zhang, Haiyan Chen, et al. "Abstract 2885: O-carborane-entrapped polymeric Micelles for Proton Boron Capture Therapy." Cancer Research 84, no. 6_Supplement (2024): 2885. http://dx.doi.org/10.1158/1538-7445.am2024-2885.

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Abstract Introduction: Proton boron capture therapy (PBCT) has the potential to enhance the biological effectiveness of proton therapy, based on proton-boron fusion reactions (11B + p → 3α + 8.7 MeV), which produce 3 α particles. In this study, we formulated o-carborane, a high boron content cage-like compound, into a polymeric micelle (M-carb) as a delivery tool to achieve effective delivery of the boronated compound to cancer cells and validated the enhancement of the biological effectiveness of proton therapy promoted by the uptake of o-carborane-entrapped in the micelle. Methods: O-carbora
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35

Jung, Joo-Young, Do-Kun Yoon, Brendan Barraclough, Heui Chang Lee, Tae Suk Suh, and Bo Lu. "Comparison between proton boron fusion therapy (PBFT) and boron neutron capture therapy (BNCT): a Monte Carlo study." Oncotarget 8, no. 24 (2017): 39774–81. http://dx.doi.org/10.18632/oncotarget.15700.

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36

Santos, Daniel, Nadine Sauzet, Olivier Guillaudin, and Jean-François Muraz. "Neutron spectroscopy from 1 to 15 MeV with Mimac-FastN, a mobile and directional fast neutron spectrometer and an active phantom for BNCT and PFBT." EPJ Web of Conferences 231 (2020): 05003. http://dx.doi.org/10.1051/epjconf/202023105003.

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In the frame of direct dark matter search, the fast neutrons producing elastic collisions on the nuclei of the active volume are the ultimate background. The MIMAC (MIcro-tpc MAtrix Chambers) project has developed a directional detector providing the directional signature to discriminate them from the searched events based on 3D nuclear tracks reconstruction. The MIMAC team of the LPSC has adapted one MIMAC chamber as a mobile fast neutron spectrometer, the Mimac-FastN detector, having a wide neutron energy range (10 keV – 600 MeV) working with different gas mixtures and pressures. This presen
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37

Dimitrijević, Milan S., Magdalena D. Christova, and Sylvie Sahal-Bréchot. "Data on Stark Broadening of N VI Spectral Lines." Data 9, no. 6 (2024): 77. http://dx.doi.org/10.3390/data9060077.

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Data on Stark broadening parameters, spectral line widths, and shifts for 15 multiplets of N VI, whose spectral lines are broadened by collisions with electrons, protons, alpha particles (He III) and B III, B IV, B V and B VI ions, are presented. They have been calculated using the semiclassical perturbation theory, for temperatures from 50,000 K to 2,000,000 K, and perturber densities from 1016 cm−3 up to 1024 cm−3. The data for e, p and He III are of particular interest for the analysis and modelling of atmospheres of hot and dense stars, as, e.g., white dwarfs, and for investigation of thei
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38

Meyer, Henry J., Uwe Titt, and Radhe Mohan. "Technical note: Monte Carlo study of the mechanism of proton–boron fusion therapy." Medical Physics 49, no. 1 (2021): 579–82. http://dx.doi.org/10.1002/mp.15381.

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Jung, J., D. Yoon, H. Shin, M. Kim, and T. Suh. "SU-D-304-07: Application of Proton Boron Fusion Reaction to Radiation Therapy." Medical Physics 42, no. 6 (2015): 3209. http://dx.doi.org/10.1118/1.4923866.

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40

Petringa, G., G. A. P. Cirrone, C. Caliri, et al. "Prompt gamma-ray emission for future imaging applications in proton-boron fusion therapy." Journal of Instrumentation 12, no. 03 (2017): C03059. http://dx.doi.org/10.1088/1748-0221/12/03/c03059.

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41

Picciotto, Antonino, Matteo Valt, Daniel P. Molloy, et al. "Ammonia borane-based targets for new developments in laser-driven proton boron fusion." Applied Surface Science 672 (November 2024): 160797. http://dx.doi.org/10.1016/j.apsusc.2024.160797.

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42

Kurilenkov, Yurii, Vladimir Tarakanov, Alexander Oginov, Sergei Gus’kov, and Igor Samoylov. "On the plasma quasineutrality under oscillatory confinement based on a nanosecond vacuum discharge." Applied Physics, no. 6 (December 24, 2021): 14–23. http://dx.doi.org/10.51368/1996-0948-2021-6-14-23.

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One of the main problems for inertial electrostatic confinement devices with electron injection is the space charge neutralization. This work is devoted to the analysis of the problem of plasma quasineutrality in the scheme of plasma oscillatory confinement based on nanosecond vacuum discharge (NVD). Electrodynamics modeling of the processes of aneutronic fusion of proton–boron showed that the plasma in the NVD, and especially on the discharge axis, really corresponds to a quasineutral regime, which is rather different from the well-known scheme of periodically oscillating plasma spheres (POPS
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43

Yoon, Do-Kun, Joo-Young Jung, and Tae Suk Suh. "Application of proton boron fusion reaction to radiation therapy: A Monte Carlo simulation study." Applied Physics Letters 105, no. 22 (2014): 223507. http://dx.doi.org/10.1063/1.4903345.

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44

Geser, Federico Alejandro, and Mauro Valente. "A theoretical model for the cross section of the proton-boron fusion nuclear reaction." Radiation Physics and Chemistry 167 (February 2020): 108224. http://dx.doi.org/10.1016/j.radphyschem.2019.03.028.

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45

Hora, H., G. H. Miley, N. Azizi, B. Malekynia, M. Ghoranneviss, and X. T. He. "Nonlinear force driven plasma blocks igniting solid density hydrogen boron: Laser fusion energy without radioactivity." Laser and Particle Beams 27, no. 3 (2009): 491–96. http://dx.doi.org/10.1017/s026303460999022x.

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AbstractEnergy production by laser driven fusion energy is highly matured by spherical compression and ignition of deuterium-tritium (DT) fuel. An alternative scheme is the fast ignition where petawatt (PW)-picosecond (ps) laser pulses are used. A significant anomaly was measured and theoretically analyzed with very clean PW-ps laser pulses for avoiding relativistic self focusing. This permits a come-back of the side-on ignition scheme of uncompressed solid DT, which is in essential contrast to the spherical compression scheme. The conditions of side-on ignition thresholds needed exorbitantly
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46

Yoon, D., J. Jung, H. Shin, M. Kim, H. Jang, and T. Suh. "SU-E-T-656: Quantitative Analysis of Proton Boron Fusion Therapy (PBFT) in Various Conditions." Medical Physics 42, no. 6Part22 (2015): 3487. http://dx.doi.org/10.1118/1.4925019.

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47

Hora, Heinrich, Shalom Eliezer, Noaz Nissim, and Paraskevas Lalousis. "Non-thermal laser driven plasma-blocks for proton boron avalanche fusion as direct drive option." Matter and Radiation at Extremes 2, no. 4 (2017): 177–89. http://dx.doi.org/10.1016/j.mre.2017.05.001.

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48

Shin, Han-Back, Do-Kun Yoon, Joo-Young Jung, Moo-Sub Kim, and Tae Suk Suh. "Prompt gamma ray imaging for verification of proton boron fusion therapy: A Monte Carlo study." Physica Medica 32, no. 10 (2016): 1271–75. http://dx.doi.org/10.1016/j.ejmp.2016.05.053.

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49

Mehlhorn, Thomas A., Lance Labun, Bjorn Manuel Hegelich, et al. "Path to Increasing p-B11 Reactivity via ps and ns Lasers." Laser and Particle Beams 2022 (December 24, 2022): 1–16. http://dx.doi.org/10.1155/2022/2355629.

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The Lawson criterion for proton-boron (p-11B) thermonuclear fusion is substantially higher than that for deuterium-tritium (DT) because the fusion cross section is lower and peaks at higher ion energies. The Maxwellian averaged p-11B reactivity peaks at several hundred keV, where bremsstrahlung radiation emission may dominate over fusion reactions if electrons and ions are in thermal equilibrium and the losses are unrestricted. Nonequilibrium burn has often been suggested to realize the benefits of this aneutronic reaction, but the predominance of elastic scattering over fusion reactivity make
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Shin, H., D. Yoon, J. Jung, M. Kim, H. Jang, and T. Suh. "MO-F-CAMPUS-J-05: Verification for Prompt Gamma Ray Imaging During Proton Boron Fusion Therapy." Medical Physics 42, no. 6Part30 (2015): 3583. http://dx.doi.org/10.1118/1.4925485.

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