Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam
Intense pulsed neutron fluences are generated by a high-energy (>10 MeV) proton beam using the beam-target method on the HERMES III facility at Sandia National Laboratories [J. J. Ramirez et al., in Proceedings of the 7th International Conference on High Power Particle Beams (Kernforschungszentru...
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| Format: | Article |
| Language: | English |
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AIP Publishing LLC
2020-12-01
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| Series: | AIP Advances |
| Online Access: | http://dx.doi.org/10.1063/5.0023480 |
| _version_ | 1818427048430927872 |
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| author | T. J. Renk P. F. Ottinger R. E. Durrer |
| author_facet | T. J. Renk P. F. Ottinger R. E. Durrer |
| author_sort | T. J. Renk |
| collection | DOAJ |
| description | Intense pulsed neutron fluences are generated by a high-energy (>10 MeV) proton beam using the beam-target method on the HERMES III facility at Sandia National Laboratories [J. J. Ramirez et al., in Proceedings of the 7th International Conference on High Power Particle Beams (Kernforschungszentrum, Karlsruhe GmbH, Karlsruhe, Germany, 1988), p. 148]. In order to generate the high-energy proton beam, a radial ion diode previously developed and fielded at the 6-MeV level in negative polarity was extended in performance to the 15-MeV level. This performance increase is described along with the development of a more durable hardware set to withstand the much more potent 15-MeV proton beam. An extensive series of simulations is developed to characterize the neutrons produced by the proton–target interaction. Particle-in-cell simulations describe the electron and ion dynamics, while Monte Carlo simulations characterize the neutron output. Due to differing estimates of proton beam voltage and current between the respective simulations, we make an approximate estimate of 13.5-MeV to 15-MeV and 120-kA ion beams at peak power in a 40 ns FWHM pulse. Simulations indicate that a total of 1.7 × 1013 neutrons are generated into 4π. Comparison of the neutron output predictions with a limited set of neutron flux measurements suggests a flux level of ∼1 × 1010 neutrons/cm2 to 10 × 1010 neutrons/cm2 over an approximately few tens of cm2 area at the relevant application location. This effort also contributes to physics understanding of the use of inductive voltage adder platforms to drive ion-beam diode loads. |
| first_indexed | 2024-12-14T14:39:32Z |
| format | Article |
| id | doaj.art-8f77cf35e3b242c79db6f735821d8502 |
| institution | Directory Open Access Journal |
| issn | 2158-3226 |
| language | English |
| last_indexed | 2024-12-14T14:39:32Z |
| publishDate | 2020-12-01 |
| publisher | AIP Publishing LLC |
| record_format | Article |
| series | AIP Advances |
| spelling | doaj.art-8f77cf35e3b242c79db6f735821d85022022-12-21T22:57:28ZengAIP Publishing LLCAIP Advances2158-32262020-12-011012125106125106-1910.1063/5.0023480Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beamT. J. Renk0P. F. Ottinger1R. E. Durrer2Sandia National Laboratories, Albuquerque, New Mexico 87185, USASyntek Technologies, Fairfax, Virginia 22031, USASigma Science, Inc., Albuquerque, New Mexico 87110, USAIntense pulsed neutron fluences are generated by a high-energy (>10 MeV) proton beam using the beam-target method on the HERMES III facility at Sandia National Laboratories [J. J. Ramirez et al., in Proceedings of the 7th International Conference on High Power Particle Beams (Kernforschungszentrum, Karlsruhe GmbH, Karlsruhe, Germany, 1988), p. 148]. In order to generate the high-energy proton beam, a radial ion diode previously developed and fielded at the 6-MeV level in negative polarity was extended in performance to the 15-MeV level. This performance increase is described along with the development of a more durable hardware set to withstand the much more potent 15-MeV proton beam. An extensive series of simulations is developed to characterize the neutrons produced by the proton–target interaction. Particle-in-cell simulations describe the electron and ion dynamics, while Monte Carlo simulations characterize the neutron output. Due to differing estimates of proton beam voltage and current between the respective simulations, we make an approximate estimate of 13.5-MeV to 15-MeV and 120-kA ion beams at peak power in a 40 ns FWHM pulse. Simulations indicate that a total of 1.7 × 1013 neutrons are generated into 4π. Comparison of the neutron output predictions with a limited set of neutron flux measurements suggests a flux level of ∼1 × 1010 neutrons/cm2 to 10 × 1010 neutrons/cm2 over an approximately few tens of cm2 area at the relevant application location. This effort also contributes to physics understanding of the use of inductive voltage adder platforms to drive ion-beam diode loads.http://dx.doi.org/10.1063/5.0023480 |
| spellingShingle | T. J. Renk P. F. Ottinger R. E. Durrer Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam AIP Advances |
| title | Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam |
| title_full | Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam |
| title_fullStr | Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam |
| title_full_unstemmed | Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam |
| title_short | Production of pulsed high-energy neutron bursts from beam–target interaction using a 15 MeV HERMES III ion beam |
| title_sort | production of pulsed high energy neutron bursts from beam target interaction using a 15 mev hermes iii ion beam |
| url | http://dx.doi.org/10.1063/5.0023480 |
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