Hiroshi Gota
Research Subjects
Hiroshi Gota has a total of 425 co-authors. Here are the top co-authors by number of shared publications:
- Tomohiko Asai
Nihon University
24 shared publications M. Tuszewski
TAE Technologies, Inc., Foothill Ranch, USA
16 shared publicationsT. Tajima
TAE Technologies, Inc., Foothill Ranch, USA
13 shared publications- Thomas Roche
TAE Technologies, Inc., Foothill Ranch, CA, United States of America
13 shared publications B. H. Deng
Tri Alpha Energy, Inc. , P.O. Box 7010, Rancho Santa Margarita, California 92688, USA
12 shared publications- Matthew C Thompson
TAE Technologies, Inc., Foothill Ranch, California 92610, USA
10 shared publications
Latest Publications
- Open Access
- 6 August 2026
- Published by Cambridge University Press (CUP) in Journal of Plasma Physics
- Vol. 92 (4) , E107
Parallel shock-relevant whistler waves and reflected ions driven by a coaxial plasma gun
A flexible laboratory configuration on the Big Red Ball device has been created for studying the physics of parallel shock formation by firing a coaxial plasma gun into a pre-existing plasma along the direction of the background magnetic field. At Alfvén Mach numbers near upper M Subscript upper A Baseline tilde 2.4 $M_A \sim 2.4$ , we observe this plasma gun piston initiate a dispersive whistler pulse and reflect ions that are collisionless against the background. These reflected ions are focused into an on-axis bunch by a concave-forward potential structure specific to the cylindrical geometry. Resonance of these reflected ions with the dispersive whistler waves, though not observed in the experiment, is a potential mechanism for collisionless shock formation.- 6 August 2026
- Published by Cambridge University Press (CUP) in Journal of Plasma Physics
- Vol. 92 (4) , E107
Open AccessParallel shock-relevant whistler waves and reflected ions driven by a coaxial plasma gun
A flexible laboratory configuration on the Big Red Ball device has been created for studying the physics of parallel shock formation by firing a coaxial plasma gun into a pre-existing plasma along the direction of the background magnetic field. At Alfvén Mach numbers near upper M Subscript upper A Baseline tilde 2.4 $M_A \sim 2.4$ , we observe this plasma gun piston initiate a dispersive whistler pulse and reflect ions that are collisionless against the background. These reflected ions are focused into an on-axis bunch by a concave-forward potential structure specific to the cylindrical geometry. Resonance of these reflected ions with the dispersive whistler waves, though not observed in the experiment, is a potential mechanism for collisionless shock formation. - Open Access
- 21 January 2026
- Published by IOP Publishing in Nuclear Fusion
- Vol. 66 (3)
Increased p- 11 B fusion reaction rate through fast-ion acceleration by ion cyclotron range of frequencies heating in LHD
Proton-boron-11 (p- 11 B) fusion is an attractive concept for advanced fusion energy because of its nearly aneutronic characteristics. However, efficient use of beam-injected fast ions may be limited by their slowing down through Coulomb collisions, which lead to lower fusion reactivity. In this study we investigate whether ion cyclotron range of frequencies (ICRF) heating can ameliorate this effect by resonantly accelerating fast ions in the Large Helical Device (LHD) of a stellarator. Using the tangential neutral beam (NB) injection to supply energetic protons at ∼160-170 keV, together with boron seeding, we conducted a series of experiments with superimposed hydrogen minority ICRF heating for beam proton acceleration. Three complementary experimental methods, ICRF power modulation, NB termination, and NB energy scan, consistently showed that ICRF waves accelerate beam ions and enhance the p- 11 B fusion yield. This led to measurable enhancements in the p- 11 B fusion alpha-particle yield, as observed with a dedicated fusion-product detector. These findings provide the first direct experimental evidence that ICRF heating can improve the efficiency of beam-driven p- 11 B fusion reactions.
- 21 January 2026
- Published by IOP Publishing in Nuclear Fusion
- Vol. 66 (3)
Open AccessIncreased p- 11 B fusion reaction rate through fast-ion acceleration by ion cyclotron range of frequencies heating in LHD
Proton-boron-11 (p- 11 B) fusion is an attractive concept for advanced fusion energy because of its nearly aneutronic characteristics. However, efficient use of beam-injected fast ions may be limited by their slowing down through Coulomb collisions, which lead to lower fusion reactivity. In this study we investigate whether ion cyclotron range of frequencies (ICRF) heating can ameliorate this effect by resonantly accelerating fast ions in the Large Helical Device (LHD) of a stellarator. Using the tangential neutral beam (NB) injection to supply energetic protons at ∼160-170 keV, together with boron seeding, we conducted a series of experiments with superimposed hydrogen minority ICRF heating for beam proton acceleration. Three complementary experimental methods, ICRF power modulation, NB termination, and NB energy scan, consistently showed that ICRF waves accelerate beam ions and enhance the p- 11 B fusion yield. This led to measurable enhancements in the p- 11 B fusion alpha-particle yield, as observed with a dedicated fusion-product detector. These findings provide the first direct experimental evidence that ICRF heating can improve the efficiency of beam-driven p- 11 B fusion reactions.
- Top Cited PapersOpen Access
- 12 April 2025
- Published by Springer Nature in Nature Communications
- Vol. 16 (1) , 1-11
Generation of field-reversed configurations via neutral beam injection
We report evidence of successful generation of field-reversed configuration plasmas by neutral beam injection. This is achieved by trapping the steady-state beams in an initial seed plasma, hence providing a direct source of toroidally directed energetic ion current and increase plasma density and temperature until plasma and magnetic pressures become comparable. Magnetic flux trapping occurs gradually, and the change in topology from open field line to fully a formed field-reversed configuration is complete within ~ 10 ms. Field reversal is first established using a traditional metric and complemented by advanced reconstruction algorithms of the magnetic topology and plasma pressure profiles; observations of characteristic changes to fast-ion orbits inferred from magnetic fluctuations; and an experimentally validated model of field reversal by neutral beam injection. These results establish a field-reversed configuration formation method which may offer technological and economic advantages on a path to a future fusion energy system.
- 12 April 2025
- Published by Springer Nature in Nature Communications
- Vol. 16 (1) , 1-11
Top Cited PapersOpen AccessGeneration of field-reversed configurations via neutral beam injection
We report evidence of successful generation of field-reversed configuration plasmas by neutral beam injection. This is achieved by trapping the steady-state beams in an initial seed plasma, hence providing a direct source of toroidally directed energetic ion current and increase plasma density and temperature until plasma and magnetic pressures become comparable. Magnetic flux trapping occurs gradually, and the change in topology from open field line to fully a formed field-reversed configuration is complete within ~ 10 ms. Field reversal is first established using a traditional metric and complemented by advanced reconstruction algorithms of the magnetic topology and plasma pressure profiles; observations of characteristic changes to fast-ion orbits inferred from magnetic fluctuations; and an experimentally validated model of field reversal by neutral beam injection. These results establish a field-reversed configuration formation method which may offer technological and economic advantages on a path to a future fusion energy system.
- 12 March 2025
- Published by Taylor & Francis in Fusion Science and Technology
- Vol. 82 (7) , 1-16
Advancing Fusion Research and Development at TAE Technologies Through INFUSE Program
- 12 March 2025
- Published by Taylor & Francis in Fusion Science and Technology
- Vol. 82 (7) , 1-16
Advancing Fusion Research and Development at TAE Technologies Through INFUSE Program
- Open Access
- 23 August 2024
- Published by IOP Publishing in Nuclear Fusion
- Vol. 64 (11) , 112014
Enhanced plasma performance in C-2W advanced beam-driven field-reversed configuration experiments
TAE Technologies’ fifth-generation fusion device, C-2W (also called ‘Norman’), is the world’s largest compact-toroid device and has made significant progress in field-reversed configuration (FRC) plasma performance. C-2W produces record breaking, macroscopically stable, high-temperature advanced beam-driven FRC plasmas, dominated by injected fast particles and sustained in steady state, which is primarily limited by neutral-beam (NB) pulse duration. The NB power supply system has recently been upgraded to extend the pulse length from 30 ms to 40 ms, which allows for a longer plasma lifetime and thus better characterization and further enhancement of FRC performance. An active plasma control system is routinely used in C-2W to produce consistent FRC performance as well as for reliable machine operations using magnet coils, edge-biasing electrodes, gas injection and tunable-energy NBs. Google’s machine learning framework for experimental optimization has also been routinely used to enhance plasma performance. Dedicated plasma optimization experimental campaigns, particularly focused on the external magnetic field profile and NB injection (NBI) optimizations, have produced a superior FRC plasma performance; for instance, achieving a total plasma energy of ∼13 kJ, a trapped poloidal magnetic flux of ∼16 mWb (based on the rigid-rotor model) and plasma sustainment in steady state up to ∼40 ms. Furthermore, under some operating conditions, the electron temperature of FRC plasmas at a quiescent phase has successfully reached up to ∼1 keV at the peak inside the FRC separatrix for the first time. The overall FRC performance is well correlated with the NB and edge-biasing systems, where higher total plasma energy is obtained with higher NBI power and applied voltage on biasing electrodes. C-2W operations have now reached a mature level where the machine can produce hot, stable, long-lived, and repeatable plasmas in a well-controlled manner.
- 23 August 2024
- Published by IOP Publishing in Nuclear Fusion
- Vol. 64 (11) , 112014
Open AccessEnhanced plasma performance in C-2W advanced beam-driven field-reversed configuration experiments
TAE Technologies’ fifth-generation fusion device, C-2W (also called ‘Norman’), is the world’s largest compact-toroid device and has made significant progress in field-reversed configuration (FRC) plasma performance. C-2W produces record breaking, macroscopically stable, high-temperature advanced beam-driven FRC plasmas, dominated by injected fast particles and sustained in steady state, which is primarily limited by neutral-beam (NB) pulse duration. The NB power supply system has recently been upgraded to extend the pulse length from 30 ms to 40 ms, which allows for a longer plasma lifetime and thus better characterization and further enhancement of FRC performance. An active plasma control system is routinely used in C-2W to produce consistent FRC performance as well as for reliable machine operations using magnet coils, edge-biasing electrodes, gas injection and tunable-energy NBs. Google’s machine learning framework for experimental optimization has also been routinely used to enhance plasma performance. Dedicated plasma optimization experimental campaigns, particularly focused on the external magnetic field profile and NB injection (NBI) optimizations, have produced a superior FRC plasma performance; for instance, achieving a total plasma energy of ∼13 kJ, a trapped poloidal magnetic flux of ∼16 mWb (based on the rigid-rotor model) and plasma sustainment in steady state up to ∼40 ms. Furthermore, under some operating conditions, the electron temperature of FRC plasmas at a quiescent phase has successfully reached up to ∼1 keV at the peak inside the FRC separatrix for the first time. The overall FRC performance is well correlated with the NB and edge-biasing systems, where higher total plasma energy is obtained with higher NBI power and applied voltage on biasing electrodes. C-2W operations have now reached a mature level where the machine can produce hot, stable, long-lived, and repeatable plasmas in a well-controlled manner.
- Open Access
- 2 August 2024
- Published by IOP Publishing in Nuclear Fusion
- Vol. 64 (9) , 096028
Demonstration of aneutronic p-11B reaction in a magnetic confinement device
Aneutronic fusion using commonly available fuel such as hydrogen and boron 11 (11B) is one of the most attractive potential energy sources. On the other hand, it requires 30 times higher temperature than deuterium–tritium fusion in a thermonuclear fusion reactor condition. Development of techniques to realize its potential for the experimental capability to produce proton-boron 11 (p-11B) fusion in the magnetically confined fusion device using neutral beam injection is desired. Here we report clear experimental exploration and measurements of p-11B fusion reactions supported by intense hydrogen beams and impurity powder dropper installed in the magnetic confinement plasma Large Helical Device. We measured a significant amount of fusion alpha particle emission using a custom designed alpha particle detector based on a passivated implanted planar silicon detector. Intense negative-ion-based hydrogen beam injectors created a large population of up to 160 keV energetic protons to react with the boron-injected plasma. The p-11B alpha particles having MeV energy were measured with the alpha particle detector which gave a fusion rate in a good agreement with the global p-11B alpha emission rate calculated based on classical confinement of energetic proton, using experimentally obtained plasma parameters.
- 2 August 2024
- Published by IOP Publishing in Nuclear Fusion
- Vol. 64 (9) , 096028
Open AccessDemonstration of aneutronic p-11B reaction in a magnetic confinement device
Aneutronic fusion using commonly available fuel such as hydrogen and boron 11 (11B) is one of the most attractive potential energy sources. On the other hand, it requires 30 times higher temperature than deuterium–tritium fusion in a thermonuclear fusion reactor condition. Development of techniques to realize its potential for the experimental capability to produce proton-boron 11 (p-11B) fusion in the magnetically confined fusion device using neutral beam injection is desired. Here we report clear experimental exploration and measurements of p-11B fusion reactions supported by intense hydrogen beams and impurity powder dropper installed in the magnetic confinement plasma Large Helical Device. We measured a significant amount of fusion alpha particle emission using a custom designed alpha particle detector based on a passivated implanted planar silicon detector. Intense negative-ion-based hydrogen beam injectors created a large population of up to 160 keV energetic protons to react with the boron-injected plasma. The p-11B alpha particles having MeV energy were measured with the alpha particle detector which gave a fusion rate in a good agreement with the global p-11B alpha emission rate calculated based on classical confinement of energetic proton, using experimentally obtained plasma parameters.
- Open Access
- 26 July 2024
- Published by IOP Publishing in Nuclear Fusion
- Vol. 64 (9) , 096013
Refueling of field-reversed configuration core via axial plasmoids injection
This study successfully developed a refueling technique for a field-reversed configuration (FRC) via axial plasmoid injection and demonstrated it on the FAT-CM device at Nihon University. The target FRC is generated using the collisional-merging formation technique combined with conical theta-pinch formation. Plasmoids with an FRC-like configuration are coaxially injected from both ends of the FAT-CM device toward the preexisting target FRC. Postinjection, the system achieves equilibrium, resulting in increases by factors of 1.8 and 2.4 in the total inventory and plasma energy, respectively, compared to cases without injection. This method effectively accomplishes FRC refueling while preserving the intrinsic characteristics of a simply connected, axisymmetric configuration and a high beta value approaching unity. Therefore, this approach offers potential for repetitive refueling in the reactor stage having a FRC plasma core. Experimental outcomes are compared with magnetohydrodynamic simulation results. In the collisional merging process, the characteristics of the pre-collision plasmoids, such as the strong toroidal rotation and coherent FRC-like magnetic field structures of the FRC, are not preserved. Experimental environments have been constructed to investigate such unique properties of the resulting FRCs.
- 26 July 2024
- Published by IOP Publishing in Nuclear Fusion
- Vol. 64 (9) , 096013
Open AccessRefueling of field-reversed configuration core via axial plasmoids injection
This study successfully developed a refueling technique for a field-reversed configuration (FRC) via axial plasmoid injection and demonstrated it on the FAT-CM device at Nihon University. The target FRC is generated using the collisional-merging formation technique combined with conical theta-pinch formation. Plasmoids with an FRC-like configuration are coaxially injected from both ends of the FAT-CM device toward the preexisting target FRC. Postinjection, the system achieves equilibrium, resulting in increases by factors of 1.8 and 2.4 in the total inventory and plasma energy, respectively, compared to cases without injection. This method effectively accomplishes FRC refueling while preserving the intrinsic characteristics of a simply connected, axisymmetric configuration and a high beta value approaching unity. Therefore, this approach offers potential for repetitive refueling in the reactor stage having a FRC plasma core. Experimental outcomes are compared with magnetohydrodynamic simulation results. In the collisional merging process, the characteristics of the pre-collision plasmoids, such as the strong toroidal rotation and coherent FRC-like magnetic field structures of the FRC, are not preserved. Experimental environments have been constructed to investigate such unique properties of the resulting FRCs.
- Top Cited PapersOpen Access
- 21 February 2023
- Published by Springer Nature in Nature Communications
- Vol. 14 (1) , 1-6
First measurements of p11B fusion in a magnetically confined plasma
Proton-boron (p11B) fusion is an attractive potential energy source but technically challenging to implement. Developing techniques to realize its potential requires first developing the experimental capability to produce p11B fusion in the magnetically-confined, thermonuclear plasma environment. Here we report clear experimental measurements supported by simulation of p11B fusion with high-energy neutral beams and boron powder injection in a high-temperature fusion plasma (the Large Helical Device) that have resulted in diagnostically significant levels of alpha particle emission. The injection of boron powder into the plasma edge results in boron accumulation in the core. Three 2 MW, 160 kV hydrogen neutral beam injectors create a large population of well-confined, high -energy protons to react with the boron plasma. The fusion products, MeV alpha particles, are measured with a custom designed particle detector which gives a fusion rate in very good relative agreement with calculations of the global rate. This is the first such realization of p11B fusion in a magnetically confined plasma.
- 21 February 2023
- Published by Springer Nature in Nature Communications
- Vol. 14 (1) , 1-6
Top Cited PapersOpen AccessFirst measurements of p11B fusion in a magnetically confined plasma
Proton-boron (p11B) fusion is an attractive potential energy source but technically challenging to implement. Developing techniques to realize its potential requires first developing the experimental capability to produce p11B fusion in the magnetically-confined, thermonuclear plasma environment. Here we report clear experimental measurements supported by simulation of p11B fusion with high-energy neutral beams and boron powder injection in a high-temperature fusion plasma (the Large Helical Device) that have resulted in diagnostically significant levels of alpha particle emission. The injection of boron powder into the plasma edge results in boron accumulation in the core. Three 2 MW, 160 kV hydrogen neutral beam injectors create a large population of well-confined, high -energy protons to react with the boron plasma. The fusion products, MeV alpha particles, are measured with a custom designed particle detector which gives a fusion rate in very good relative agreement with calculations of the global rate. This is the first such realization of p11B fusion in a magnetically confined plasma.
- 1 December 2022
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 93 (12) , 123512
Development of multichord ion Doppler spectroscopy system for toroidal flow measurement of field-reversed configuration
A double-chord ion Doppler spectroscopy (IDS) system was developed to measure the ion temperature and flow velocity of field-reversed configuration (FRC) plasmas in the FRC amplification via a translation-collisional merging (FAT-CM) device. Adopting a Czerny–Turner mount monochromator and 16-channel photomultiplier tube array, the developed IDS system achieves high wavelength resolution and fast time response. In addition, two vertically aligned optical paths share the optical system up to the monochromator and then branch just before the detector, successfully reducing crosstalk to <1%. The Doppler broadening was measured at two measurement points in the FAT-CM device, simultaneously, and ion temperatures of ∼50 eV were measured. Toroidal spin-up from 7 to 15 km/s and a steady flow velocity of ∼10 km/s were estimated from the Doppler shift obtained by the developed system. The observation of the toroidal flow velocity and the spatial profile of the ion temperature of the FRC plasma in the FAT-CM device were realized. These spectroscopic diagnostic’s double chord capabilities will aid in understanding and improving the FRC plasmas.
- 1 December 2022
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 93 (12) , 123512
Development of multichord ion Doppler spectroscopy system for toroidal flow measurement of field-reversed configuration
A double-chord ion Doppler spectroscopy (IDS) system was developed to measure the ion temperature and flow velocity of field-reversed configuration (FRC) plasmas in the FRC amplification via a translation-collisional merging (FAT-CM) device. Adopting a Czerny–Turner mount monochromator and 16-channel photomultiplier tube array, the developed IDS system achieves high wavelength resolution and fast time response. In addition, two vertically aligned optical paths share the optical system up to the monochromator and then branch just before the detector, successfully reducing crosstalk to <1%. The Doppler broadening was measured at two measurement points in the FAT-CM device, simultaneously, and ion temperatures of ∼50 eV were measured. Toroidal spin-up from 7 to 15 km/s and a steady flow velocity of ∼10 km/s were estimated from the Doppler shift obtained by the developed system. The observation of the toroidal flow velocity and the spatial profile of the ion temperature of the FRC plasma in the FAT-CM device were realized. These spectroscopic diagnostic’s double chord capabilities will aid in understanding and improving the FRC plasmas.
- 1 October 2022
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 93 (10) , 103526
Spectroscopic observation of super-Alfvénic field-reversed configuration merging process by mixing of tracer ions
Visualization of the collisional merging formation process of field-reversed configuration (FRC) has been attempted. In the collisional merging formation process, two initial FRC-like plasmoids are accelerated toward each other by a magnetic pressure gradient. The relative speed of the collision reaches several times the typical ion sonic speed and Alfvénic speed. The magnetic structure of the initial-FRCs is disrupted in the collision process, but the FRC-like magnetic structure is reformed in ∼30 µs after the collision. Magnetic reconnection should occur in this process; however, general theoretical models in magnetohydrodynamics approximation cannot be applied to this process because of the high-beta nature of FRC and super-Alfvénic/sonic relative speed. In this work, the spectroscopic observation of the collisional merging FRC formation was conducted to evaluate the timescale and geometry of merging. A slight amount of tracer element (e.g., helium) was mixed into one of two initial-FRCs. Mixing of the tracer did not cause serious adverse effects on the performance of the initial-FRC in the collision and merging processes. The collision and merging processes were visualized successfully and observed using a fast-framing camera with a bandpass filter. The timescale of merging and the outflow speed in the collisional merging process of FRCs were optically evaluated for the first time.
- 1 October 2022
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 93 (10) , 103526
Spectroscopic observation of super-Alfvénic field-reversed configuration merging process by mixing of tracer ions
Visualization of the collisional merging formation process of field-reversed configuration (FRC) has been attempted. In the collisional merging formation process, two initial FRC-like plasmoids are accelerated toward each other by a magnetic pressure gradient. The relative speed of the collision reaches several times the typical ion sonic speed and Alfvénic speed. The magnetic structure of the initial-FRCs is disrupted in the collision process, but the FRC-like magnetic structure is reformed in ∼30 µs after the collision. Magnetic reconnection should occur in this process; however, general theoretical models in magnetohydrodynamics approximation cannot be applied to this process because of the high-beta nature of FRC and super-Alfvénic/sonic relative speed. In this work, the spectroscopic observation of the collisional merging FRC formation was conducted to evaluate the timescale and geometry of merging. A slight amount of tracer element (e.g., helium) was mixed into one of two initial-FRCs. Mixing of the tracer did not cause serious adverse effects on the performance of the initial-FRC in the collision and merging processes. The collision and merging processes were visualized successfully and observed using a fast-framing camera with a bandpass filter. The timescale of merging and the outflow speed in the collisional merging process of FRCs were optically evaluated for the first time.