Search citation statements
Paper Sections
Citation Types
Year Published
Publication Types
Relationship
Authors
Journals
Laser-driven ions have compelling properties and their potential use for medical applications has attracted a huge global interest. One of the major challenges of these applications is generating beams of the required energies. To date, there has been no systematic study of the effect of laser intensity on the generation of laser-driven ions from ultrathin foils during relativistic transparency. Here we present a scaling for ion energies with respect to the on-target laser intensity and in considering target thickness we find an optimum thickness closely related to the experimentally observed relativistic transparency. A steep linear scaling with the normalized laser amplitude a0 has been measured and verified with PIC simulations. In contrast to TNSA, this scaling is much steeper and has been measured for ions with Z > 1. Following our results, ion energies exceeding 100MeV/amu are already accessible with currently available laser systems enabling realization of numerous advanced applications.For more than a decade, intense short pulse lasers have been used to drive energetic ion beams [1][2][3][4][5][6][7]. These laser-driven ion beams have high particle numbers, energies up to several tens of MeV/amu [8] and a low transverse emittance [9] and a promise to be a competitive alternative to conventional radio frequency accelerators. The range of applications covers medicine with hadron cancer therapy [10], threat reduction (e.g. detection of fissile material) [11,12] or energy generation with concepts in ion fast ignition [13][14][15]. The major drawback so far is that ion energies are typically too low for any of these applications. For the hadron cancer therapy, protons of 250MeV or carbon C 6+ ions of 4-5 GeV are needed. In the regime of the Target Normal Sheath Acceleration (TNSA) [1-3] protons have been accelerated to 67MeV [16] with laser intensities exceeding 10 20 W/cm 2 . Heavier ions have merely reached several MeV/amu due to protons shielding the accelerating fields in this mechanism. Even with target cleaning, energies have not passed 10 MeV\amu [6]. Recent advances in laser intensities and contrast enabled exploration of new acceleration mechanisms such as the radiation pressure acceleration (RPA) [17][18][19][20][21] or the Break-Out Afterburner (BOA) [22][23][24][25] mechanism, which reach higher ion energies for both protons and heavier ions.Scaling laws for ion energies are a fundamental requirement for the design of future laser systems and the realization of advanced applications. So far, scaling laws have been discussed for the TNSA mechanism [5,7] and also for RPA dominated acceleration [18,27,41]. Here, we extend this research framework by presenting experimental data and theoretical analysis for scaling of ion energies in the relativistic transparent regime, where the BOA mechanism is operative. In a series of experiments we investigated how maximum ion energies scale for the BOA. Ion energies have been measured for intensities of 8 × 10 19 , 2 × 10 20 and 1.7 × 10 21 W/cm 2 at the Los Alamo...
Laser-driven ions have compelling properties and their potential use for medical applications has attracted a huge global interest. One of the major challenges of these applications is generating beams of the required energies. To date, there has been no systematic study of the effect of laser intensity on the generation of laser-driven ions from ultrathin foils during relativistic transparency. Here we present a scaling for ion energies with respect to the on-target laser intensity and in considering target thickness we find an optimum thickness closely related to the experimentally observed relativistic transparency. A steep linear scaling with the normalized laser amplitude a0 has been measured and verified with PIC simulations. In contrast to TNSA, this scaling is much steeper and has been measured for ions with Z > 1. Following our results, ion energies exceeding 100MeV/amu are already accessible with currently available laser systems enabling realization of numerous advanced applications.For more than a decade, intense short pulse lasers have been used to drive energetic ion beams [1][2][3][4][5][6][7]. These laser-driven ion beams have high particle numbers, energies up to several tens of MeV/amu [8] and a low transverse emittance [9] and a promise to be a competitive alternative to conventional radio frequency accelerators. The range of applications covers medicine with hadron cancer therapy [10], threat reduction (e.g. detection of fissile material) [11,12] or energy generation with concepts in ion fast ignition [13][14][15]. The major drawback so far is that ion energies are typically too low for any of these applications. For the hadron cancer therapy, protons of 250MeV or carbon C 6+ ions of 4-5 GeV are needed. In the regime of the Target Normal Sheath Acceleration (TNSA) [1-3] protons have been accelerated to 67MeV [16] with laser intensities exceeding 10 20 W/cm 2 . Heavier ions have merely reached several MeV/amu due to protons shielding the accelerating fields in this mechanism. Even with target cleaning, energies have not passed 10 MeV\amu [6]. Recent advances in laser intensities and contrast enabled exploration of new acceleration mechanisms such as the radiation pressure acceleration (RPA) [17][18][19][20][21] or the Break-Out Afterburner (BOA) [22][23][24][25] mechanism, which reach higher ion energies for both protons and heavier ions.Scaling laws for ion energies are a fundamental requirement for the design of future laser systems and the realization of advanced applications. So far, scaling laws have been discussed for the TNSA mechanism [5,7] and also for RPA dominated acceleration [18,27,41]. Here, we extend this research framework by presenting experimental data and theoretical analysis for scaling of ion energies in the relativistic transparent regime, where the BOA mechanism is operative. In a series of experiments we investigated how maximum ion energies scale for the BOA. Ion energies have been measured for intensities of 8 × 10 19 , 2 × 10 20 and 1.7 × 10 21 W/cm 2 at the Los Alamo...
Kinetic modeling of laser-ion beam generation from the “break-out afterburner” (BOA) has been modeled for several deuteron-rich solid-density target foils. Modeling the transport of these beams in a beryllium converter shows as much as a fourfold increase in neutron yield over the present state of the art through the use of alternative target materials. Additionally, species-separation dynamics during the BOA can be exploited to control the hardness of the neutron spectra, of interest for, for example, enhancing penetrability in shielded material in active neutron interrogation settings.
Emerging approaches to short-pulse laser-driven neutron production offer a possible gateway to compact, low cost, and intense broad spectrum sources for a wide variety of applications. They are based on energetic ions, driven by an intense short-pulse laser, interacting with a converter material to produce neutrons via breakup and nuclear reactions. Recent experiments performed with the high-contrast laser at the Trident laser facility of Los Alamos National Laboratory have demonstrated a laser-driven ion acceleration mechanism operating in the regime of relativistic transparency, featuring a volumetric laser-plasma interaction. This mechanism is distinct from previously studied ones that accelerate ions at the laser-target surface. The Trident experiments produced an intense beam of deuterons with an energy distribution extending above 100 MeV. This deuteron beam, when directed at a beryllium converter, produces a forward-directed neutron beam with ∼5 × 109 n/sr, in a single laser shot, primarily due to deuteron breakup. The neutron beam has a pulse duration on the order of a few nanoseconds with an energy distribution extending from a few hundreds of keV to almost 80 MeV. For the experiments on neutron-source spot-size measurements, our gated neutron imager was setup to select neutrons in the energy range of 2.5–35 MeV. The spot size of neutron emission at the converter was measured by two different imaging techniques, using a knife-edge and a penumbral aperture, in two different experimental campaigns. The neutron-source spot size is measured ∼1 mm for both experiments. The measurements and analysis reported here give a spatial characterization for this type of neutron source for the first time. In addition, the forward modeling performed provides an empirical estimate of the spatial characteristics of the deuteron ion-beam. These experimental observations, taken together, provide essential yet unique data to benchmark and verify theoretical work into the basic acceleration mechanism, which remains an ongoing challenge.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.
hi@scite.ai
10624 S. Eastern Ave., Ste. A-614
Henderson, NV 89052, USA
Copyright © 2024 scite LLC. All rights reserved.
Made with 💙 for researchers
Part of the Research Solutions Family.