Wikipedia

Magnetic confinement fusion

Magnetic confinement fusion (MCF) is an approach to generate thermonuclear fusion power that uses magnetic fields to confine fusion fuel in the form of a plasma. Magnetic confinement is one of two major branches of controlled fusion research, along with inertial confinement fusion.

A typical plasma in the MAST spherical tokamak machine at the Culham Centre for Fusion Energy in the UK.

Fusion reactions for reactors usually combine light atomic nuclei of deuterium and tritium to form an alpha particle (Helium-4 nucleus) and a neutron, where the energy is released in the form of the kinetic energy of the reaction products. In order to overcome the electrostatic repulsion between the nuclei, the fuel must have a temperature of hundreds of millions of degrees, at which the fuel is fully ionized and becomes a plasma. In addition, the plasma must be at a sufficient density, and the energy must remain in the reacting region for a sufficient time, as specified by the Lawson criterion (triple product). The high temperature of a fusion plasma precludes the use of material vessels for direct containment. Magnetic confinement fusion attempts to use the physics of charged particle motion to contain the plasma particles by applying strong magnetic fields.

Tokamaks and stellarators are the two leading MCF device candidates as of today. Investigation of using various magnetic configurations to confine fusion plasma began in the 1950s. Early simple mirror and toroidal machines showed disappointing results of low confinement. After the declassification of fusion research by the United States, United Kingdom and Soviet Union in 1958, a breakthrough on toroidal devices was reported by the Kurchatov Institute in 1968, where its tokamak demonstrated a temperature of 1 kilo-electronvolts (around 11.6 million degree Kelvin) and some milliseconds of confinement time, and was confirmed by a visiting team from the Culham Laboratory using the Thomson scattering technique.[1][2] Since then, tokamaks became the dominant line of research globally with large tokamaks such as JET, TFTR and JT-60 being constructed and operated. The ITER tokamak experiment under construction, which aims to demonstrate scientific breakeven, will be the world's largest MCF device. While early stellarators of low confinement in the 1950s were overshadowed by the initial success of tokamaks, interests in stellarators re-emerged attributing to their inherent capability for steady-state and disruption-free operation distinct from tokamaks. The world's largest stellarator experiment, Wendelstein 7-X, began operation in 2015.

The current record of fusion power generated by MCF devices is held by JET. In 1997, JET set the record of 16 megawatts of transient fusion power with a gain factor of Q = 0.62 and 4 megawatts steady state fusion power with Q = 0.18 for 4 seconds.[3] In 2021, JET sustained Q = 0.33 for 5 seconds and produced 59 megajoules of energy, beating the record 21.7 megajoules released in 1997 over around 4 seconds.[4]

One of the challenges of MCF research is the development and extrapolation of plasma scenarios to power plant conditions, where good fusion performance and energy confinement must be maintained. Potential solutions to other problems such as divertor power exhaust, mitigation of transients (disruptions, runaway electrons, edge-localized modes), handling of neutron flux, tritium breeding and the physics of burning plasmas are being actively studied. Development of new technologies in plasma diagnostics, real-time control, plasma-facing materials, high-power microwave sources, vacuum engineering, cryogenics and superconducting magnets are essential in MCF research.

Types

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Magnetic mirrors

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Main article: Magnetic mirror

A major area of research in the early years of fusion energy research was the magnetic mirror. Most early mirror devices attempted to confine plasma near the focus of a non-planar magnetic field generated in a solenoid with the field strength increased at either end of the tube. In order to escape the confinement area, nuclei had to enter a small annular area near each magnet. It was known that nuclei would escape through this area, but by adding and heating fuel continually it was felt this could be overcome.

In 1954, Edward Teller gave a talk in which he outlined a theoretical problem that suggested the plasma would also quickly escape sideways through the confinement fields. This would occur in any machine with convex magnetic fields, which existed in the centre of the mirror area. Existing machines were having other problems and it was not obvious whether this was occurring. In 1961, a Soviet team conclusively demonstrated this flute instability was indeed occurring, and when a US team stated they were not seeing this issue, the Soviets examined their experiment and noted this was due to a simple instrumentation error.

The Soviet team also introduced a potential solution, in the form of "Ioffe bars". These bent the plasma into a new shape that was concave at all points, avoiding the problem Teller had pointed out. This demonstrated a clear improvement in confinement. A UK team then introduced a simpler arrangement of these magnets they called the "tennis ball", which was taken up in the US as the "baseball". Several baseball series machines were tested and showed much-improved performance. However, theoretical calculations showed that the maximum amount of energy they could produce would be about the same as the energy needed to run the magnets. As a power-producing machine, the mirror appeared to be a dead end.

In the 1970s, a solution was developed. By placing a baseball coil at either end of a large solenoid, the entire assembly could hold a much larger volume of plasma, and thus produce more energy. Plans began to build a large device of this "tandem mirror" design, which became the Mirror Fusion Test Facility (MFTF). Having never tried this layout before, a smaller machine, the Tandem Mirror Experiment (TMX) was built to test this layout. TMX demonstrated a new series of problems that suggested MFTF would not reach its performance goals, and during construction MFTF was modified to MFTF-B. However, due to budget cuts, one day after the construction of MFTF was completed it was mothballed. Mirrors have seen little development since that time.

Toroidal machines

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Concept of a toroidal fusion reactor

Z-pinch

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The first real effort to build a control fusion reactor used the pinch effect in a toroidal container. A large transformer wrapping the container was used to induce a current in the plasma inside. This current creates a magnetic field that squeezes the plasma into a thin ring, thus "pinching" it. The combination of Joule heating by the current and adiabatic heating as it pinches raises the temperature of the plasma to the required range in the tens of millions of degrees Kelvin.

First built in the UK in 1948, and followed by a series of increasingly large and powerful machines in the UK and US, all early machines proved subject to powerful instabilities in the plasma. Notable among them was the kink instability, which caused the pinched ring to thrash about and hit the walls of the container long before it reached the required temperatures. The concept was so simple, however, that herculean effort was expended to address these issues.

This led to the "stabilized pinch" concept, which added external magnets to "give the plasma a backbone" while it compressed. The largest such machine was the UK's ZETA reactor, completed in 1957, which appeared to successfully produce fusion. Only a few months after its public announcement in January 1958, these claims had to be retracted when it was discovered the neutrons being seen were created by new instabilities in the plasma mass. Further studies showed any such design would be beset with similar problems, and research using the z-pinch approach largely ended.

Stellarators

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Main article: Stellarator

An early attempt to build a magnetic confinement system was the stellarator, introduced by Lyman Spitzer in 1951. Essentially the stellarator consists of a torus that has been cut in half and then attached back together with straight "crossover" sections to form a figure-8. This has the effect of propagating the nuclei from the inside to outside as it orbits the device, thereby cancelling out the drift across the axis, at least if the nuclei orbit fast enough.

Not long after the construction of the earliest figure-8 machines, it was noticed the same effect could be achieved in a completely circular arrangement by adding a second set of helically wound magnets on either side. This arrangement generated a field that extended only part way into the plasma, which proved to have the significant advantage of adding "shear", which suppressed turbulence in the plasma. However, as larger devices were built on this model, it was seen that plasma was escaping from the system much more rapidly than expected, much more rapidly than could be replaced.

By the mid-1960s it appeared the stellarator approach was a dead end. In addition to the fuel loss problems, it was also calculated that a power-producing machine based on this system would be enormous, the better part of a thousand feet (300 meters) long. When the tokamak was introduced in 1968, interest in the stellarator vanished, and the latest design at Princeton University, the Model C, was eventually converted to the Symmetrical Tokamak.

Stellarators have seen renewed interest since the turn of the millennium as they avoid several problems subsequently found in the tokamak. Newer models have been built, but these remain about two generations behind the latest tokamak designs.

Tokamaks

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Main article: Tokamak
 
Tokamak magnetic fields.

In the late 1950s, Soviet researchers noticed that the kink instability would be strongly suppressed if the twists in the path were strong enough that a particle travelled around the circumference of the inside of the chamber more rapidly than around the chamber's length. This would require the pinch current to be reduced and the external stabilizing magnets to be made much stronger.

In 1968 Russian research on the toroidal tokamak was first presented in public, with results that far outstripped existing efforts from any competing design, magnetic or not. Since then the majority of effort in magnetic confinement has been based on the tokamak principle. In the tokamak a current is periodically driven through the plasma itself, creating a field "around" the torus that combines with the toroidal field to produce a winding field in some ways similar to that in a modern stellarator, at least in that nuclei move from the inside to the outside of the device as they flow around it.

In 1991, START was built at Culham, UK, as the first purpose-built spherical tokamak. This was essentially a spheromak with an inserted central rod. START produced impressive results, with β values at approximately 40% - three times that produced by standard tokamaks at the time. The concept has been scaled up to higher plasma currents and larger sizes, with the experiments NSTX (US), MAST (UK) and Globus-M (Russia) currently running. Spherical tokamaks have improved stability properties compared to conventional tokamaks and as such the area is receiving considerable experimental attention. However, spherical tokamaks to date have been at low toroidal field and as such are impractical for fusion neutron devices.

Compact toroids

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Compact toroids, e.g. the spheromak and the Field-Reversed Configuration, attempt to combine the good confinement of closed magnetic surfaces configurations with the simplicity of machines without a central core. An early experiment of this type[dubious – discuss] in the 1970s was Trisops. (Trisops fired two theta-pinch rings towards each other.)

Other

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Some more novel configurations produced in toroidal machines are the reversed field pinch and the Levitated Dipole Experiment.

The US Navy has also claimed a "Plasma Compression Fusion Device" capable of TW power levels in a 2018 US patent filing:

"It is a feature of the present invention to provide a plasma compression fusion device that can produce power in the gigawatt to terawatt range (and higher), with input power in the kilowatt to megawatt range."[5]

However, the patent has since been abandoned.

Magnetic fusion energy

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All of these devices have faced considerable problems being scaled up and in their approach toward the Lawson criterion. One researcher has described the magnetic confinement problem in simple terms, likening it to squeezing a balloon – the air will always attempt to "pop out" somewhere else. Turbulence in the plasma has proven to be a major problem, causing the plasma to escape the confinement area, and potentially touch the walls of the container. If this happens, a process known as "sputtering", high-mass particles from the container (often steel and other metals) are mixed into the fusion fuel, lowering its temperature.

In 1997, scientists at the Joint European Torus (JET) facilities in the UK produced 16 megawatts of fusion power. Scientists can now exercise a measure of control over plasma turbulence and resultant energy leakage, long considered an unavoidable and intractable feature of plasmas. There is increased optimism that the plasma pressure above which the plasma disassembles can now be made large enough to sustain a fusion reaction rate acceptable for a power plant.[6] Electromagnetic waves can be injected and steered to manipulate the paths of plasma particles and then to produce the large electrical currents necessary to produce the magnetic fields to confine the plasma.[7] These and other control capabilities have come from advances in basic understanding of plasma science in such areas as plasma turbulence, plasma macroscopic stability, and plasma wave propagation. Much of this progress has been achieved with a particular emphasis on the tokamak.

Recent developments

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Cutaway view of the current design for the SPARC reactor

SPARC is a tokamak using deuterium–tritium (DT) fuel, currently being designed at the MIT Plasma Science and Fusion Center in collaboration with Commonwealth Fusion Systems with the goal of producing a practical reactor design in the near future. In late 2020, a special issue of the Journal of Plasma Physics was published including seven studies speaking to a high level of confidence in the efficacy of the reactor design focusing on using simulations to validate predictions for the operation and capacity of the reactor.[8] One study focused on modeling the magnetohydrodynamic (MHD) conditions in the reactor. The stability of this condition will define the limits of plasma pressure that can be achieved under varying magnetic field pressures.[9]

The progress made with SPARC has built off previously mentioned work on the ITER project and is aiming to utilize new technology in high-temperature superconductors (HTS) as a more practical material. HTS will enable reactor magnets to produce greater magnetic field and proportionally increase the transport processes necessary to generate energy. One of the largest material considerations is ensuring the inner wall will be able to handle the intense amounts of heat that will be generated (expected to approach 10 GW per square meter in heat flux from the plasma). Not only does this material need to survive, but it needs to withstand damage enough to avoid contaminating the core plasma. Challenges such as this are being actively considered and accounted for in the models and predictive calculations used in the design process.[10]

Progress has been made in addressing the challenge of core-edge integration in future fusion reactors at the DIII-D National Fusion Facility. For a burning fusion plasma, it is crucial to maintain a plasma core hotter than the Sun's surface without damaging the reactor walls. Injecting impurities heavier than the plasma particles into the plasma and power exhaust region (the Divertor) is crucial for cooling the plasma boundary without affecting the fusion performance. Conventional experiments used gaseous impurities, but the injection of boron, boron nitride, and lithium in powder form has also been tested.[11][12] Experiments showed effective cooling of the plasma boundary with minimal impact on the performance of high-confinement mode plasmas. This approach could be applied to larger fusion devices like ITER and contribute to core-edge integration in future fusion power plants.[13][14] Recent experiments have also made progress in disruption prediction, ELM control, and material migration. The program is installing additional tools to optimize tokamak operation and exploring edge plasma and materials interactions. Major upgrades are being considered to enhance performance and flexibility for future fusion reactors.[15][16][17]

The Wendelstein 7-X stellarator at the Max Planck Institute for Plasma Physics in Germany has finished its first plasma campaigns and underwent upgrades, including the installation of over 8,000 graphite wall tiles and ten divertor modules to protect the vessel walls and enable longer plasma discharges.[18][19][20] The experiments will test the optimized concept of Wendelstein 7-X as a stellarator fusion device for potential use in a power plant. The island divertor plays a crucial role in regulating plasma purity and density. Wendelstein 7-X allows the investigation into plasma turbulence and the effectiveness of magnetic confinement and thermal insulation. The device's microwave heating system has also been improved to achieve higher energy throughput and plasma density. These advancements aim to demonstrate the suitability of stellarators for continuous fusion power generation.[21][22][23][24]

TAE Technologies achieved 2022 a significant research milestone by conducting the first-ever hydrogen-boron fusion experiments in a magnetically confined fusion plasma. The experiments were conducted in collaboration with Japan's National Institute for Fusion Science using a boron powder injection system developed by scientists and engineers of the Princeton Plasma Physics Laboratory.[25][26] TAE's pursuit of hydrogen-boron fusion aims to develop a clean, cost-competitive, and sustainable fuel cycle for fusion power. The results suggest that a hydrogen-boron fuel mix has the potential to be used in utility-scale fusion power. TAE Technologies is focused on developing a fusion power plant by the mid-2030s that will produce clean electricity.[27]

The private U.S. nuclear fusion company Helion Energy has signed a deal with Microsoft to provide electricity in about five years, marking the first such agreement for fusion power. Helion's plant, expected to be online by 2028, aims to generate 50 megawatts or more of power. The company plans to use helium-3, a rare gas as a fuel source.[28]

Kronos Fusion Energy has announced the development of an aneutronic fusion energy generator for clean and limitless power in national defense.[29]

In May 2023, the United States Department of Energy (DOE) announced a $46 million grant for eight companies across seven states to advance fusion power plant designs and research, aiming to establish the U.S. as a leader in clean fusion energy. The funding from the Milestone-Based Fusion Development Program supports the goal to demonstrate pilot-scale fusion within ten years and achieve a net-zero economy by 2050. The grant recipients will tackle scientific and technological hurdles to create viable fusion pilot plant designs in the next 5–10 years. The awardees include Commonwealth Fusion Systems, Focused Energy Inc., Princeton Stellarators Inc., Realta Fusion Inc., Tokamak Energy Inc., Type One Energy Group, Xcimer Energy Inc., and Zap Energy Inc.[30]

Experimental laboratories

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The world's major magnetic confinement fusion laboratories are:

See also

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References

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  1. ^ Peacock, N. J.; Robinson, D. C.; Forrest, M. J.; Wilcock, P. D.; Sannikov, V. V. (November 1969). "Measurement of the Electron Temperature by Thomson Scattering in Tokamak T3". Nature. 224 (5218): 488–490. Bibcode:1969Natur.224..488P. doi:10.1038/224488a0. ISSN 0028-0836. S2CID 4290094.
  2. ^ Holloway, Nick (2019-11-22). "Mission to Moscow: 50 years on". Culham Centre for Fusion Energy. Retrieved 2023-08-22.
  3. ^ Keilhacker, M; Gibson, A; Gormezano, C; Rebut, P.H (December 2001). "The scientific success of JET". Nuclear Fusion. 41 (12): 1925–1966. doi:10.1088/0029-5515/41/12/217. ISSN 0029-5515. S2CID 250759123.
  4. ^ Gibney, Elizabeth (2022-02-09). "Nuclear-fusion reactor smashes energy record". Nature. 602 (7897): 371. Bibcode:2022Natur.602..371G. doi:10.1038/d41586-022-00391-1. PMID 35140372.
  5. ^ "Plasma Compression Fusion Device".
  6. ^ ITER Physics Expert Group on Energetic Particles, Heating and Current Drive; ITER Physics Basis Editors (1999). "Chapter 6: Plasma auxiliary heating and current drive". Nuclear Fusion. 39 (12): 2495–2539. Bibcode:1999NucFu..39.2495I. doi:10.1088/0029-5515/39/12/306.
  7. ^ "Radio-frequency wave scattering improves fusion simulations". Mit News | Massachusetts Institute of Technology. Retrieved 2022-01-25.
  8. ^ Scott, S. D.; Kramer, G. J.; Tolman, E. A.; Snicker, A.; Varje, J.; Särkimäki, K.; Wright, J. C.; Rodriguez-Fernandez, P. (2020). "Fast-ion physics in SPARC". Journal of Plasma Physics. 86 (5): 865860508. Bibcode:2020JPlPh..86e8608S. doi:10.1017/S0022377820001087. ISSN 0022-3778. S2CID 224975897.
  9. ^ Sweeney, R.; Creely, A. J.; Doody, J.; Fülöp, T.; Garnier, D. T.; Granetz, R.; Greenwald, M.; Hesslow, L.; Irby, J.; Izzo, V. A.; La Haye, R. J. (2020). "MHD stability and disruptions in the SPARC tokamak". Journal of Plasma Physics. 86 (5): 865860507. Bibcode:2020JPlPh..86e8607S. doi:10.1017/S0022377820001129. ISSN 0022-3778. S2CID 224869796.
  10. ^ Kuang, A. Q.; Ballinger, S.; Brunner, D.; Canik, J.; Creely, A. J.; Gray, T.; Greenwald, M.; Hughes, J. W.; Irby, J.; LaBombard, B.; Lipschultz, B. (2020). "Divertor heat flux challenge and mitigation in SPARC". Journal of Plasma Physics. 86 (5): 865860505. Bibcode:2020JPlPh..86e8605K. doi:10.1017/S0022377820001117. hdl:1721.1/136124. ISSN 0022-3778. S2CID 224847975.
  11. ^ Casali, L; Eldon, D; et al. (2022). "Impurity leakage and radiative cooling in the first nitrogen and neon seeding study in the closed DIII-D SAS configuration". Nucl. Fusion. 62 (2): 026021. Bibcode:2022NucFu..62b6021C. doi:10.1088/1741-4326/ac3e84. OSTI 1863590. S2CID 244820223.
  12. ^ Effenberg, F; Bortolon, A; Casali, L; Nazikian, R; et al. (2022). "Mitigation of plasma–wall interactions with low-Z powders in DIII-D high confinement plasmas". Nucl. Fusion. 62 (10): 106015. arXiv:2203.15204. Bibcode:2022NucFu..62j6015E. doi:10.1088/1741-4326/ac899d. S2CID 247778852.
  13. ^ Andrei, Mihai (2021-11-08). "Fusion breakthrough brings us one step closer to solving key challenges". ZME Science. Archived from the original on 2021-11-08. Retrieved 2021-11-08.
  14. ^ "Integrating hot cores and cool edges in fusion reactors". ZME Science. American Physical Society. 2021-11-08. Archived from the original on 2023-04-29. Retrieved 2021-11-08.
  15. ^ "DIII-D National Fusion Facility Begins Transformation to Prepare for Future Reactors" (Press release). 18 May 2018. Retrieved 15 May 2023.
  16. ^ "Creating a star on Earth: Nuclear fusion program at General Atomics gets 5-year extension". 12 November 2019. Retrieved 15 May 2023.
  17. ^ Fenstermacher, M. E.; Abbate, J.; Abe, S. (1 April 2022). "DIII-D research advancing the physics basis for optimizing the tokamak approach to fusion energy". Nuclear Fusion. 62 (4): 042024. doi:10.1088/1741-4326/ac2ff2. hdl:1721.1/147629. S2CID 244608556.
  18. ^ "Wendelstein 7-X: Second round of experimentation started". 6 December 2016. Retrieved 11 September 2017.
  19. ^ Sunn Pedersen, T.; Andreeva, T.; Bosch, H. -S; Bozhenkov, S.; Effenberg, F.; Endler, M.; Feng, Y.; Gates, D. A.; Geiger, J.; Hartmann, D.; Hölbe, H.; Jakubowski, M.; König, R.; Laqua, H. P.; Lazerson, S.; Otte, M.; Preynas, M.; Schmitz, O.; Stange, T.; Turkin, Y. (November 2015). "T. Sunn Pedersen et al 2015 Nucl. Fusion 55 126001". Nuclear Fusion. 55 (12): 126001. doi:10.1088/0029-5515/55/12/126001. hdl:11858/00-001M-0000-0029-04EB-D. S2CID 67798335.
  20. ^ BrezƖnsek, S.; Dhard, C.P.; Jakubowski, M. (1 January 2022). "Plasma–surface interaction in the stellarator W7-X: conclusions drawn from operation with graphite plasma-facing components". Nuclear Fusion. 62 (1): 016006. doi:10.1088/1741-4326/ac3508. S2CID 240484560.
  21. ^ Pedersen, T. Sunn; Otte, M.; Lazerson, S.; et al. (2016). "Confirmation of the topology of the Wendelstein 7-X magnetic field to better than 1:100,000". Nature Communications. 7: 13493. Bibcode:2016NatCo...713493P. doi:10.1038/ncomms13493. PMC 5141350. PMID 27901043.
  22. ^ "Tests confirm that Germany's massive nuclear fusion machine really works". ScienceAlert. 6 December 2016. Retrieved 7 December 2016.
  23. ^ Wolf, R. C.; et al. (27 July 2017). "R.C. Wolf et al 2017 Nucl. Fusion 57 102020". Nuclear Fusion. 57 (10): 102020. doi:10.1088/1741-4326/aa770d. hdl:2434/616000. S2CID 1986901.
  24. ^ Wolf, R. C.; Alonso, A.; Äkäslompolo, S.; et al. (1 August 2019). "Performance of Wendelstein 7-X stellarator plasmas during the first divertor operation phase". Physics of Plasmas. 26 (8): 082504. Bibcode:2019PhPl...26h2504W. doi:10.1063/1.5098761. hdl:1721.1/130063. S2CID 202127809.
  25. ^ "TAE makes world-first readings of magnetically-confined hydrogen-boron fusion". 28 February 2023. Retrieved 15 May 2023.
  26. ^ Nagy, A.; Bortolon, A.; Mauzey, D. M.; Wolfe, E.; Gilson, E. P.; Lunsford, R.; Maingi, R.; Mansfield, D. K.; Nazikian, R.; Roquemore, A. L. (2018). "A. Nagy et al Rev Sci Instrum 89, 10K121 (2018)". The Review of Scientific Instruments. 89 (10): 10K121. doi:10.1063/1.5039345. OSTI 1485110. PMID 30399718. S2CID 53225855.
  27. ^ "Google and Chevron invest in nuclear fusion startup that's raised $1.2 billion". CNBC. 20 July 2022. Retrieved 15 May 2023.
  28. ^ Gardner, Timothy (10 May 2023). "Microsoft signs power purchase deal with nuclear fusion company Helion". Reuters. Retrieved 15 May 2023.
  29. ^ "Kronos Fusion Energy Aims for Fully Commercialized Fusion Generators by 2032" (Press release). 10 August 2022. Retrieved 15 May 2023.
  30. ^ "US announces $46 million in funds to eight nuclear fusion companies" (Press release). 31 May 2023. Retrieved 13 June 2023.
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