This timeline of nuclear fusion is an incomplete chronological summary of significant events in the study and use of
nuclear fusion.
1920s
1920
Based on
F.W. Aston's measurements of the masses of low-mass elements and
Einstein's discovery that E=mc2,
Arthur Eddington proposes that large amounts of energy released by
fusing small nuclei together provides the energy source that powers the stars.[1]
Henry Norris Russell notes that the relationship in the
Hertzsprung–Russell diagram suggests a hot core rather than burning throughout the star. Eddington uses this to calculate that the core would have to be about 40 million Kelvin. This was a matter of some debate at the time, because the value is much higher than what observations suggest, which is about one-third to one-half that value.
Atkinson and
Houtermans provide the first calculations of the rate of nuclear fusion in stars. Based on Gamow's tunnelling, they show fusion can occur at lower energies than previously believed. When used with Eddington's calculations of the required fusion rates in stars, their calculations demonstrate this would occur at the lower temperatures that Eddington had calculated.[3]
In April, Walton produces the first man-made fission by using
protons from the accelerator to split
lithium into
alpha particles.[4]
Using an updated version of the equipment firing deuterium rather than hydrogen,
Mark Oliphant discovered
helium-3 and
tritium, and that heavy
hydrogen nuclei could be made to react with each other.[5]This is the first direct demonstration of fusion in the lab.
1938
Kantrowitz and Jacobs of the
NACALangley Research Center built a toroidal
magnetic bottle and heat the plasma with a 150 W radio source. Hoping to heat the plasma to millions of degrees, the system fails and they are forced to abandon their
Diffusion Inhibitor.[6]This is the first attempt to make a working fusion reactor.
1939
Peter Thonemann develops a detailed plan for a
pinch device, but is told to do other work for his thesis.[6]
A meeting at
Harwell on the topic of fusion raises new concerns with the concept. On his return to London, Thomson gets graduate students
James L. Tuck and
Alan Alfred Ware to build a prototype device out of old radar parts.[9]
Peter Thonemann comes up with a similar idea, but uses a different method of heating the fuel. This seems much more practical and finally gains the mild interest of the UK nuclear establishment. Not aware of who he is talking to, Thonemann describes the concept to Thomson, who adopts the same concept.[9]
Herbert Skinner begins to write a lengthy report on the entire fusion concept, pointing out several areas of little or no knowledge.[9]
1948
The
Ministry of Supply (MoS) asks Thomson about the status of his patent filing, and he describes the problems he has getting funding. The MoS forces Harwell to provide some money, and Thomson releases his rights to the patent. It is granted late that year.[9]
Skinner publishes his report, calling for some experimental effort to explore the areas of concern. Along with the MoS's calls for funding of Thomson, this event marks the beginning of formal fusion research in the UK.[9]
1950s
1950
In January,
Klaus Fuchs admits to passing nuclear secrets to the
Soviet Union. Almost all nuclear research in the UK, including the fledgling fusion program, is immediately classified. Thomson, until this time working at Imperial University, is moved to the
Atomic Weapons Research Establishment.
A press release from
Argentina claims that their
Huemul Project had produced controlled nuclear fusion. This prompted a wave of responses in other countries, especially the U.S.
Tuck introduces the British pinch work to LANL. He develops the
Perhapsatron under the codename
Project Sherwood. The project name is a play on his name via Friar Tuck.[10]
In the UK, repeated requests for more funding that had previously been turned down are suddenly approved. Within a short time, three separate efforts are started, one at Harwell and two at
Atomic Weapons Establishment (Aldermaston). Early planning for a much larger machine at Harwell begins.
Using the Huemul release as leverage, Soviet researchers find their funding proposals rapidly approved. Work on linear pinch machines begins that year.
Cousins and Ware build a larger toroidal
pinch device in England and demonstrated that the plasma in pinch devices is inherently unstable.
1953
The Soviet RDS-6S test, code named "
Joe 4", demonstrated a fission/fusion/fission ("Layercake") design for a nuclear weapon.
Linear pinch devices in the US and USSR report detections of
neutrons, an indication of fusion reactions. Both are later explained as coming from instabilities in the fuel, and are non-fusion in nature.
1954
Early planning for the large
ZETA device at Harwell begins. The name is a take-off on
small experimental fission reactors which often had "zero energy" in their name,
ZEEP being an example.
Edward Teller gives a now-famous speech on plasma stability in magnetic bottles at the Princeton Gun Club. His work suggests that most magnetic bottles are inherently unstable, outlining what is today known as the
interchange instability.
1955
At the first
Atoms for Peace meeting in Geneva,
Homi J. Bhabha predicts that fusion will be in commercial use within two decades. This prompts a number of countries to begin fusion research;
Japan,
France and
Sweden all start programs this year or the next.
Igor Kurchatov gives a talk at Harwell on pinch devices,[11] revealing for the first time that the USSR is also working on fusion. He details the problems they are seeing, mirroring those in the US and UK.
In August, a number of articles on plasma physics appear in various Soviet journals.
In the wake of the Kurchatov's speech, the US and UK begin to consider releasing their own data. Eventually, they settle on a release prior to the 2nd
Atoms for Peace conference in
Geneva in 1958.
1957
In the US, at
LANL,
Scylla I[12] begins operation using the θ-pinch design.
ZETA is completed in the summer, it will be the largest fusion machine for a decade.
In August, initial results on ZETA appear to suggest the machine has successfully reached basic fusion temperatures. UK researchers start pressing for public release, while the US demurs.
Scientists at the AEI Research laboratory in Harwell reported that the
Sceptre III plasma column remained stable for 300 to 400 microseconds, a dramatic improvement on previous efforts. Working backward, the team calculated that the plasma had an electrical resistivity around 100 times that of copper, and was able to carry 200 kA of current for 500 microseconds in total.
1958
In January, the US and UK release large amounts of data, with the ZETA team claiming fusion. Other researchers, notably Artsimovich and Spitzer, are sceptical.
In May, a series of new tests demonstrate the measurements on ZETA were erroneous, and the claims of fusion have to be retracted.
American, British and
Soviet scientists began to share previously classified controlled fusion research as part of the
Atoms for Peace conference in
Geneva in September. It is the largest international scientific meeting to date. It becomes clear that basic pinch concepts are not successful and that no device has yet created fusion at any level.
Scylla demonstrates the first controlled thermonuclear fusion in any laboratory,[13][14] although confirmation came too late to be announced at Geneva. This
θ-pinch approach will ultimately be abandoned as calculations show it cannot scale up to produce a reactor.
1960s
1960
After considering the concept for some time,
John Nuckolls publishes the concept of
inertial confinement fusion. The
laser, introduced the same year, appears to be a suitable "driver".
Plasma temperatures of approximately 40 million degrees Celsius and a few billion deuteron-deuteron fusion reactions per discharge were achieved at
LANL with the
Scylla IV device.[15]
1965
At an international meeting at the UK's new fusion research centre in Culham, the Soviets release early results showing greatly improved performance in toroidal pinch machines. The announcement is met by scepticism, especially by the UK team who's ZETA was largely identical. Spitzer, chairing the meeting, essentially dismisses it out of hand.
At the same meeting, odd results from the ZETA machine are published. It will be years before the significance of these results are realized.
By the end of the meeting, it is clear that most fusion efforts have stalled. All of the major designs, including the
stellarator, pinch machines and
magnetic mirrors are all losing plasma at rates that are simply too high to be useful in a reactor setting. Less-known designs like the
levitron and
astron are faring no better.
The 12-beam "4 pi laser" using ruby as the lasing medium is developed at
Lawrence Livermore National Laboratory (LLNL) includes a gas-filled target chamber of about 20 centimeters in diameter.
1967
Demonstration of
Farnsworth-Hirsch Fusor appeared to generate neutrons in a nuclear reaction.
Further results from the T-3
tokamak, similar to the toroidal pinch machine mentioned in 1965, claims temperatures to be over an order of magnitude higher than any other device. The Western scientists remain highly sceptical.
The Soviets invite a UK team from ZETA to perform independent measurements on T-3.
1969
The UK team, nicknamed "The Culham Five", confirm the Soviet results early in the year. They publish their results in October's edition of Nature. This leads to a "veritable stampede" of tokamak construction around the world.
After learning of the Culham Five's results in August, a furious debate breaks out in the US establishment over whether or not to build a tokamak. After initially pooh-poohing the concept, the Princeton group eventually decides to convert their stellarator to a tokamak.
1970s
1970
Princeton's conversion of the
Model C stellarator to the
Symmetrical Tokamak is completed, and tests match and then best the Soviet results. With an apparent solution to the magnetic bottle problem in-hand, plans begin for a larger machine to test the scaling and various methods to heat the plasma.
Kapchinskii and Teplyakov introduce a
particle accelerator for heavy ions that appear suitable as an ICF driver in place of lasers.
1972
The first neodymium-
doped glass (Nd:glass) laser for ICF research, the "
Long Path laser" is completed at LLNL and is capable of delivering ~50 joules to a fusion target.
1973
Design work on
JET, the Joint European Torus, begins.
1974
J.B. Taylor re-visited ZETA results of 1958 and explained that the quiet-period was in fact very interesting. This led to the development of
reversed field pinch, now generalised as "self-organising plasmas", an ongoing line of research.
KMS Fusion, a private-sector company, builds an ICF reactor using laser drivers. Despite limited resources and numerous business problems, KMS successfully compresses fuel in December 1973, and on 1 May 1974 successfully demonstrates the world's first laser-induced fusion. Neutron-sensitive nuclear emulsion detectors, developed by Nobel Prize winner
Robert Hofstadter, were used to provide evidence of this discovery.
Beams using mature high-energy accelerator technology are hailed as the elusive "brand-X" driver capable of producing fusion implosions for commercial power. The
Livingston Curve, which illustrates the improvement in power of
particle accelerators over time, is modified to show the energy needed for fusion to occur. Experiments commence on the single beam LLNL
Cyclops laser, testing new optical designs for future ICF lasers.
1975
The
Princeton Large Torus (PLT), the follow-on to the Symmetrical Tokamak, begins operation. It soon surpasses the best Soviet machines and sets several temperature records that are above what is needed for a commercial reactor. PLT continues to set records until it is decommissioned.
1976
Workshop, called by the US-ERDA (now DoE) at the Claremont Hotel in Berkeley, CA for an ad-hoc two-week summer study. Fifty senior scientists from the major US ICF programs and accelerator laboratories participated, with program heads and Nobel laureates also attending. In the closing address, Dr. C. Martin Stickley, then Director of US-ERDA's Office of Inertial Fusion, announced the conclusion was "no showstoppers" on the road to fusion energy.
The two beam
Argus laser is completed at LLNL and experiments involving more advanced laser-target interactions commence.
Based on the continued success of the PLT, the DOE selects a larger Princeton design for further development. Initially designed simply to test a commercial-sized tokamak, the DOE team instead gives them the explicit goal of running on a deuterium-tritium fuel as opposed to test fuels like hydrogen or deuterium. The project is given the name
Tokamak Fusion Test Reactor (TFTR).
1977
The 20 beam
Shiva laser at LLNL is completed, capable of delivering 10.2 kilojoules of infrared energy on target. At a price of $25 million and a size approaching that of a football field, the Shiva laser is the first of the "megalasers" at LLNL and brings the field of ICF research fully within the realm of "
big science".
The
JET project is given the go-ahead by the
EC, choosing the UK's center at Culham as its site.
1978
As PLT continues to set new records, Princeton is given additional funding to adapt TFTR with the explicit goal of reaching breakeven.
1979
LANL successfully demonstrates the radio frequency quadrupole accelerator (RFQ).
ANL and Hughes Research Laboratories demonstrate required ion source brightness with xenon beam at 1.5MeV.
The Foster Panel report to US-DoE's Energy Research and advisory board on ICF concludes that
heavy ion fusion (HIF) is the "conservative approach" to ICF. Listing HIF's advantages in his report, John Foster remarked: "...now that is kind of exciting." After DoE Office of Inertial Fusion completed review of programs, Director Gregory Canavan decides to accelerate the HIF effort.
1980s
1982
HIBALL study by German and US institutions,[17] Garching uses the high repetition rate of the RF accelerator driver to serve four reactor chambers and first-wall protection using liquid lithium inside the chamber cavity.
Tore Supra construction starts at
Cadarache, France. Its
superconducting magnets will permit it to generate a strong permanent toroidal magnetic field.[18]
JET, the largest operational magnetic confinement plasma physics experiment is completed on time and on budget. First plasmas achieved.
The
NOVETTE laser at LLNL comes on line and is used as a test bed for the next generation of ICF lasers, specifically the
NOVA laser.
1984
The huge 10 beam
NOVA laser at LLNL is completed and switches on in December. NOVA would ultimately produce a maximum of 120 kilojoules of infrared laser light during a nanosecond pulse in a 1989 experiment.
1985
National Academy of Sciences reviewed military ICF programs, noting HIF's major advantages clearly but averring that HIF was "supported primarily by other [than military] programs".[citation needed] The review of ICF by the National Academy of Sciences marked the trend with the observation: "The energy crisis is dormant for the time being." Energy becomes the sole purpose of heavy ion fusion.
The Japanese tokamak,
JT-60 completed. First plasmas achieved.
1988
The
T-15, Soviet tokamak with superconducting helium-cooled coils completed.
The Conceptual Design Activity for the International Thermonuclear Experimental Reactor (
ITER), the successor to
T-15,
TFTR,
JET and
JT-60, begins.[19] Participants include
EURATOM, Japan, the
Soviet Union and United States. It ended in 1990.
On March 23, two
Utah electrochemists,
Stanley Pons and
Martin Fleischmann, announced that they had achieved
cold fusion: fusion reactions which could occur at room temperatures. However, they made their announcements before any peer review of their work was performed, and no subsequent experiments by other researchers revealed any evidence of fusion.
The
START Tokamak fusion experiment begins in
Culham. The experiment would eventually achieve a record
beta (plasma pressure compared to magnetic field pressure) of 40% using a
neutral beam injector. It was the first design that adapted the conventional toroidal fusion experiments into a tighter spherical design.
The Engineering Design Activity for the
ITER starts with participants
EURATOM, Japan, Russia and United States. It ended in 2001.
The United States and the former republics of the Soviet Union cease nuclear weapons testing.
1993
The
TFTR tokamak at
Princeton (PPPL) experiments with a 50%
deuterium, 50%
tritium mix, eventually producing as much as 10 megawatts of power from a controlled fusion reaction.
1994
NIF Beamlet laser is completed and begins experiments validating the expected performance of NIF.
The USA declassifies information about indirectly driven (hohlraum) target design.
Comprehensive European-based study of HIF driver begins, centered at the Gesellschaft für Schwerionenforschung (GSI) and involving 14 laboratories, including USA and Russia. The Heavy Ion Driven Inertial Fusion (HIDIF) study will be completed in 1997.
1996
A record is reached at
Tore Supra: a plasma duration of two minutes with a current of almost 1 million amperes driven non-inductively by 2.3 MW of
lower hybrid frequency waves (i.e. 280 MJ of injected and extracted energy). This result was possible due to the actively cooled plasma-facing components installed in the machine.[22]
The
JET tokamak in the UK produces 16 MW of fusion power - this remains the world record for fusion power until 2022 when JET sets an even higher record. Four megawatts of
alpha particle self-heating was achieved.
LLNL study compared projected costs of power from ICF and other fusion approaches to the projected future costs of existing energy sources.
The
JT-60 tokamak in Japan produced a high performance reversed shear plasma with the equivalent fusion amplification factor of 1.25 - the current world record of
Q, fusion energy gain factor.
Results of European-based study of heavy ion driven fusion power system (HIDIF, GSI-98-06) incorporates telescoping beams of multiple isotopic species. This technique multiplies the 6-D phase space usable for the design of HIF drivers.
1999
The United States withdraws from the
ITER project.
Building construction for the immense 192-beam 500-terawatt
NIF project is completed and construction of laser beam-lines and target bay diagnostics commences, expecting to take its first full system shot in 2010.
Negotiations on the Joint Implementation of
ITER begin between Canada, countries represented by the
European Union, Japan and Russia.
2002
Claims and counter-claims are published regarding
bubble fusion, in which a table-top apparatus was reported as producing small-scale fusion in a liquid undergoing
acoustic cavitation. Like cold fusion (see 1989), it is later dismissed.
The United States drops its own ITER-scale tokamak project,
FIRE, recognising an inability to match EU progress.[23]
2005
Following final negotiations between the EU and Japan,
ITER chooses
Cadarache over
Rokkasho for the site of the reactor. In concession, Japan is able to host the related materials research facility and granted rights to fill 20% of the project's research posts while providing 10% of the funding.
The
NIF fires its first bundle of eight beams achieving the highest ever energy laser pulse of 152.8 kJ (infrared).
2006
China's
EAST test reactor is completed, the first tokamak experiment to use superconducting magnets to generate both the toroidal and poloidal fields.
HIF-2010 Symposium in Darmstadt, Germany. Robert J Burke presented on Single Pass (Heavy Ion Fusion) HIF and Charles Helsley made a presentation on the commercialization of HIF within the decade.
2011
May 23–26, Workshop for Accelerators for Heavy Ion Fusion at Lawrence Berkeley National Laboratory, presentation by Robert J. Burke on "Single Pass Heavy Ion Fusion". The Accelerator Working Group publishes recommendations supporting moving RF accelerator driven HIF toward commercialization.[citation needed]
2012
Stephen Slutz & Roger Vesey of Sandia National Labs publish a paper in Physical Review Letters presenting a computer simulation of the
MagLIF concept showing it can produce high gain. According to the simulation, a 70 Mega Amp Z-pinch facility in combination with a Laser may be able to produce a spectacular energy return of 1000 times the expended energy. A 60 MA facility would produce a 100x yield.[24]
In August Robert J. Burke presents updates to the
SPRFDHIF process[25] and Charles Helsley presents the Economics of SPRFD[26] at the 19th International HIF Symposium at
Berkeley, California. Industry was there in support of ion generation for SPRFD. The Fusion Power Corporation SPRFD patent is granted in Russia.
2013
China's
EAST tokamak test reactor achieves a record confinement time of 30 seconds for plasma in the
high-confinement mode (H-mode), thanks to improvements in heat dispersal from tokamak walls. This is an improvement of an order of magnitude with respect to state-of-the-art reactors.[27]
US Scientists at
NIF successfully generate more energy from fusion reactions than the energy absorbed by the nuclear fuel.[28]
Phoenix Nuclear Labs announces the sale of a high-yield neutron generator that could sustain 5×1011deuterium fusion reactions per second over a 24-hour period.[29]
On 9 October 2014, fusion research bodies from European Union member states and Switzerland signed an agreement to cement European collaboration on fusion research and EUROfusion, the European Consortium for the Development of Fusion Energy, was born.[30]
2015
Germany conducts the first plasma discharge in
Wendelstein 7-X, a large-scale stellarator capable of steady-state plasma confinement under fusion conditions.[31]
In August,
MIT announces the
ARC fusion reactor, a compact tokamak using
rare-earth barium-copper oxide (REBCO) superconducting tapes to produce high-magnetic field coils that it claims produce comparable magnetic field strength in a smaller configuration than other designs.[33]
2016
The Wendelstein 7-X produces the device's first hydrogen plasma.[34]
2017
China's
EAST tokamak test reactor achieves a stable 101.2-second steady-state high confinement plasma, setting a world record in long-pulse H-mode operation on the night of July 3.[35]
Helion Energy's fifth-generation plasma machine goes into operation, seeking to achieve plasma density of 20 Tesla and fusion temperatures.[36]
UK company
Tokamak Energy's ST40 fusion reactor generates first plasma.[37]
MIT scientists formulate a theoretical means to remove the excess heat from compact nuclear fusion reactors via larger and longer
divertors.[42]
General Fusion begins developing a 70% scale demo system to be completed around 2023.[36]
TAE Technologies announces its reactor has reached a high temperature of nearly 20 million°C.[43]
The Fusion Industry Association founded as an initiative in 2018, is the unified voice of the fusion industry, working to transform the energy system with commercially viable fusion power.[44]
2019
The United Kingdom announces a planned £200-million (US$248-million) investment to produce a design for the
Spherical Tokamak for Energy Production (STEP) fusion facility around 2040.[45][46]
2020s
2020
Assembly of
ITER, which has been under construction for years, commences.[47]
The Chinese experimental
nuclear fusion reactor
HL-2M is turned on for the first time, achieving its first plasma discharge.[48]
2021
Record China's
EAST tokamak sets a new world record for superheated plasma, sustaining a temperature of 120 million degrees Celsius for 101 seconds and a peak of 160 million degrees Celsius for 20 seconds.[49]
Record The
National Ignition Facility achieves generating 70% of the input energy, necessary to sustain fusion, from
inertial confinementfusion energy, an 8x improvement over previous experiments in spring 2021 and a 25x increase over the yields achieved in 2018.[50]
The first Fusion Industry Association report was published - "The global fusion industry in 2021"[51]
Record China's
Experimental Advanced Superconducting Tokamak (EAST), a nuclear fusion reactor research facility, sustained plasma at 70 million degrees Celsius for as long as 1,056 seconds (17 minutes, 36 seconds), achieving the new world record for sustained high temperatures (fusion energy however requires i.a. temperatures over 150 million °C).[52][53][54]
2022
Record The
Joint European Torus in Oxford, UK, reports 59 megajoules produced with nuclear fusion over five seconds (11 megawatts of power), more than double the previous record of 1997.[55][56]
Record United States researchers at
Lawrence Livermore National Laboratory National Ignition Facility (NIF) in California has recorded the first case of ignition on August 8, 2021. Producing an energy yield of 0.72, of laser beam input to fusion output.[57][58]
Record Building on the achievement in August 2022, American researchers at
Lawrence Livermore National Laboratory National Ignition Facility (NIF) in California recorded the first ever net energy production with nuclear fusion, producing more fusion energy than laser beam put in. Laser efficiency was in the order of 1%.[59]
2023
Record On February 15, 2023,
Wendelstein 7-X reached a new milestone: Power plasma with gigajoule energy turnover generated for eight minutes.[60]
JT-60SA achieves first plasma in October, making it the largest operational superconducting tokamak in the world.[61]
2024
The Korea Superconducting Tokamak Advanced Research (
KSTAR) achieved the new record of 102-sec-long operation (Integrated RMP control for ELM-less H-mode with a notable advancement on the favorable control the error field,[62] Tungsten divertor) with the achieved duration of 48 seconds at the high-temperature of about 100 million degrees Celsius in February 2024, after the last record of 45-sec-long operation (ELM-less H-mode (FIRE mode[63]), Carbon-based divertor, 2022). See
"핵융합 플라스마 장기간 운전기술 확보 청신호, 보도자료, KSTAR연구본부" (in Korean). 20 March 2024. and
"[공식발표] 한국 인공태양 KSTAR 또 해냈다! "1억도○○ 초?"". YouTube (in Korean). (21 March 2024).
^Nimtz, G.; Clegg, B. (12 August 2009). Greenberger, D.; Hentschel, K.; Weinert, F. (eds.). Compendium of Quantum Physics. Springer. pp. 799–802.
ISBN978-3-540-70622-9.
^...the first money to be allocated [to controlled nuclear research] happened to be for Tuck, and was diverted from Project Lincoln, in the Hood Laboratory. The coincidence of names prompted the well-known cover name "Project Sherwood". James L. Tuck,
"Curriculum Vita and Autobiography", declassified document from Los Alamos National Laboratory (1974), reproduced with permission.
Archived 9 February 2012.
^"Lecture of I.V. Kurchatov at Harwell", from the address of I.V. Kurchatov: "On the possibility of producing thermonuclear reactions in a gas discharge" at Harwell on 25 April 1956.
Archived 20 July 2015.
^"Hans Bethe". Hans Bethe - Biographical. Nobel Prize.org. Retrieved 11 March 2016.
^...Gesellschaft für Schwerionenforschung; Institut für Plasmaphysik, Garching; Kernforschungszentrum Karlsruhe, University of Wisconsin, Madison; Max-Planck-Institut für Quantenoptik
^"Tore Supra". www-drfc.cea.fr. Archived from
the original on 15 November 2012. Retrieved 15 January 2022.
^那珂研究所 (1991). Annual report of the Naka Fusion Research Establishment for the period of April 1, 1990 to March 31, 1991 (Report) (in Japanese). 日本原子力研究開発機構.
doi:
10.11484/jaeri-m-91-159.
^Burke, Robert (1 January 2014). "The Single Pass RF Driver: Final beam compression". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 733: 158–167.
Bibcode:
2014NIMPA.733..158B.
doi:
10.1016/j.nima.2013.05.080.
^Helsley, Charles E.; Burke, Robert J. (January 2014). "Economic viability of large-scale fusion systems". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 733: 51–56.
Bibcode:
2014NIMPA.733...51H.
doi:
10.1016/j.nima.2013.05.095.
^ S.M.Yang et al., Tailoring tokamak error fields to control plasma instabilities and transport, Nature Communications,
10 February 2024,
https://doi.org/10.1038/s41467-024-45454-1
^ H.Han et al., A sustained high-temperature fusion plasma regime facilitated by fast ions, Nature 609, 8 September 2022, 269-275. doi:10.1038/s41586-022-05008-1.
Bibliography
Dean, Stephen (2013). Search for the Ultimate Energy Source. Springer.
This timeline of nuclear fusion is an incomplete chronological summary of significant events in the study and use of
nuclear fusion.
1920s
1920
Based on
F.W. Aston's measurements of the masses of low-mass elements and
Einstein's discovery that E=mc2,
Arthur Eddington proposes that large amounts of energy released by
fusing small nuclei together provides the energy source that powers the stars.[1]
Henry Norris Russell notes that the relationship in the
Hertzsprung–Russell diagram suggests a hot core rather than burning throughout the star. Eddington uses this to calculate that the core would have to be about 40 million Kelvin. This was a matter of some debate at the time, because the value is much higher than what observations suggest, which is about one-third to one-half that value.
Atkinson and
Houtermans provide the first calculations of the rate of nuclear fusion in stars. Based on Gamow's tunnelling, they show fusion can occur at lower energies than previously believed. When used with Eddington's calculations of the required fusion rates in stars, their calculations demonstrate this would occur at the lower temperatures that Eddington had calculated.[3]
In April, Walton produces the first man-made fission by using
protons from the accelerator to split
lithium into
alpha particles.[4]
Using an updated version of the equipment firing deuterium rather than hydrogen,
Mark Oliphant discovered
helium-3 and
tritium, and that heavy
hydrogen nuclei could be made to react with each other.[5]This is the first direct demonstration of fusion in the lab.
1938
Kantrowitz and Jacobs of the
NACALangley Research Center built a toroidal
magnetic bottle and heat the plasma with a 150 W radio source. Hoping to heat the plasma to millions of degrees, the system fails and they are forced to abandon their
Diffusion Inhibitor.[6]This is the first attempt to make a working fusion reactor.
1939
Peter Thonemann develops a detailed plan for a
pinch device, but is told to do other work for his thesis.[6]
A meeting at
Harwell on the topic of fusion raises new concerns with the concept. On his return to London, Thomson gets graduate students
James L. Tuck and
Alan Alfred Ware to build a prototype device out of old radar parts.[9]
Peter Thonemann comes up with a similar idea, but uses a different method of heating the fuel. This seems much more practical and finally gains the mild interest of the UK nuclear establishment. Not aware of who he is talking to, Thonemann describes the concept to Thomson, who adopts the same concept.[9]
Herbert Skinner begins to write a lengthy report on the entire fusion concept, pointing out several areas of little or no knowledge.[9]
1948
The
Ministry of Supply (MoS) asks Thomson about the status of his patent filing, and he describes the problems he has getting funding. The MoS forces Harwell to provide some money, and Thomson releases his rights to the patent. It is granted late that year.[9]
Skinner publishes his report, calling for some experimental effort to explore the areas of concern. Along with the MoS's calls for funding of Thomson, this event marks the beginning of formal fusion research in the UK.[9]
1950s
1950
In January,
Klaus Fuchs admits to passing nuclear secrets to the
Soviet Union. Almost all nuclear research in the UK, including the fledgling fusion program, is immediately classified. Thomson, until this time working at Imperial University, is moved to the
Atomic Weapons Research Establishment.
A press release from
Argentina claims that their
Huemul Project had produced controlled nuclear fusion. This prompted a wave of responses in other countries, especially the U.S.
Tuck introduces the British pinch work to LANL. He develops the
Perhapsatron under the codename
Project Sherwood. The project name is a play on his name via Friar Tuck.[10]
In the UK, repeated requests for more funding that had previously been turned down are suddenly approved. Within a short time, three separate efforts are started, one at Harwell and two at
Atomic Weapons Establishment (Aldermaston). Early planning for a much larger machine at Harwell begins.
Using the Huemul release as leverage, Soviet researchers find their funding proposals rapidly approved. Work on linear pinch machines begins that year.
Cousins and Ware build a larger toroidal
pinch device in England and demonstrated that the plasma in pinch devices is inherently unstable.
1953
The Soviet RDS-6S test, code named "
Joe 4", demonstrated a fission/fusion/fission ("Layercake") design for a nuclear weapon.
Linear pinch devices in the US and USSR report detections of
neutrons, an indication of fusion reactions. Both are later explained as coming from instabilities in the fuel, and are non-fusion in nature.
1954
Early planning for the large
ZETA device at Harwell begins. The name is a take-off on
small experimental fission reactors which often had "zero energy" in their name,
ZEEP being an example.
Edward Teller gives a now-famous speech on plasma stability in magnetic bottles at the Princeton Gun Club. His work suggests that most magnetic bottles are inherently unstable, outlining what is today known as the
interchange instability.
1955
At the first
Atoms for Peace meeting in Geneva,
Homi J. Bhabha predicts that fusion will be in commercial use within two decades. This prompts a number of countries to begin fusion research;
Japan,
France and
Sweden all start programs this year or the next.
Igor Kurchatov gives a talk at Harwell on pinch devices,[11] revealing for the first time that the USSR is also working on fusion. He details the problems they are seeing, mirroring those in the US and UK.
In August, a number of articles on plasma physics appear in various Soviet journals.
In the wake of the Kurchatov's speech, the US and UK begin to consider releasing their own data. Eventually, they settle on a release prior to the 2nd
Atoms for Peace conference in
Geneva in 1958.
1957
In the US, at
LANL,
Scylla I[12] begins operation using the θ-pinch design.
ZETA is completed in the summer, it will be the largest fusion machine for a decade.
In August, initial results on ZETA appear to suggest the machine has successfully reached basic fusion temperatures. UK researchers start pressing for public release, while the US demurs.
Scientists at the AEI Research laboratory in Harwell reported that the
Sceptre III plasma column remained stable for 300 to 400 microseconds, a dramatic improvement on previous efforts. Working backward, the team calculated that the plasma had an electrical resistivity around 100 times that of copper, and was able to carry 200 kA of current for 500 microseconds in total.
1958
In January, the US and UK release large amounts of data, with the ZETA team claiming fusion. Other researchers, notably Artsimovich and Spitzer, are sceptical.
In May, a series of new tests demonstrate the measurements on ZETA were erroneous, and the claims of fusion have to be retracted.
American, British and
Soviet scientists began to share previously classified controlled fusion research as part of the
Atoms for Peace conference in
Geneva in September. It is the largest international scientific meeting to date. It becomes clear that basic pinch concepts are not successful and that no device has yet created fusion at any level.
Scylla demonstrates the first controlled thermonuclear fusion in any laboratory,[13][14] although confirmation came too late to be announced at Geneva. This
θ-pinch approach will ultimately be abandoned as calculations show it cannot scale up to produce a reactor.
1960s
1960
After considering the concept for some time,
John Nuckolls publishes the concept of
inertial confinement fusion. The
laser, introduced the same year, appears to be a suitable "driver".
Plasma temperatures of approximately 40 million degrees Celsius and a few billion deuteron-deuteron fusion reactions per discharge were achieved at
LANL with the
Scylla IV device.[15]
1965
At an international meeting at the UK's new fusion research centre in Culham, the Soviets release early results showing greatly improved performance in toroidal pinch machines. The announcement is met by scepticism, especially by the UK team who's ZETA was largely identical. Spitzer, chairing the meeting, essentially dismisses it out of hand.
At the same meeting, odd results from the ZETA machine are published. It will be years before the significance of these results are realized.
By the end of the meeting, it is clear that most fusion efforts have stalled. All of the major designs, including the
stellarator, pinch machines and
magnetic mirrors are all losing plasma at rates that are simply too high to be useful in a reactor setting. Less-known designs like the
levitron and
astron are faring no better.
The 12-beam "4 pi laser" using ruby as the lasing medium is developed at
Lawrence Livermore National Laboratory (LLNL) includes a gas-filled target chamber of about 20 centimeters in diameter.
1967
Demonstration of
Farnsworth-Hirsch Fusor appeared to generate neutrons in a nuclear reaction.
Further results from the T-3
tokamak, similar to the toroidal pinch machine mentioned in 1965, claims temperatures to be over an order of magnitude higher than any other device. The Western scientists remain highly sceptical.
The Soviets invite a UK team from ZETA to perform independent measurements on T-3.
1969
The UK team, nicknamed "The Culham Five", confirm the Soviet results early in the year. They publish their results in October's edition of Nature. This leads to a "veritable stampede" of tokamak construction around the world.
After learning of the Culham Five's results in August, a furious debate breaks out in the US establishment over whether or not to build a tokamak. After initially pooh-poohing the concept, the Princeton group eventually decides to convert their stellarator to a tokamak.
1970s
1970
Princeton's conversion of the
Model C stellarator to the
Symmetrical Tokamak is completed, and tests match and then best the Soviet results. With an apparent solution to the magnetic bottle problem in-hand, plans begin for a larger machine to test the scaling and various methods to heat the plasma.
Kapchinskii and Teplyakov introduce a
particle accelerator for heavy ions that appear suitable as an ICF driver in place of lasers.
1972
The first neodymium-
doped glass (Nd:glass) laser for ICF research, the "
Long Path laser" is completed at LLNL and is capable of delivering ~50 joules to a fusion target.
1973
Design work on
JET, the Joint European Torus, begins.
1974
J.B. Taylor re-visited ZETA results of 1958 and explained that the quiet-period was in fact very interesting. This led to the development of
reversed field pinch, now generalised as "self-organising plasmas", an ongoing line of research.
KMS Fusion, a private-sector company, builds an ICF reactor using laser drivers. Despite limited resources and numerous business problems, KMS successfully compresses fuel in December 1973, and on 1 May 1974 successfully demonstrates the world's first laser-induced fusion. Neutron-sensitive nuclear emulsion detectors, developed by Nobel Prize winner
Robert Hofstadter, were used to provide evidence of this discovery.
Beams using mature high-energy accelerator technology are hailed as the elusive "brand-X" driver capable of producing fusion implosions for commercial power. The
Livingston Curve, which illustrates the improvement in power of
particle accelerators over time, is modified to show the energy needed for fusion to occur. Experiments commence on the single beam LLNL
Cyclops laser, testing new optical designs for future ICF lasers.
1975
The
Princeton Large Torus (PLT), the follow-on to the Symmetrical Tokamak, begins operation. It soon surpasses the best Soviet machines and sets several temperature records that are above what is needed for a commercial reactor. PLT continues to set records until it is decommissioned.
1976
Workshop, called by the US-ERDA (now DoE) at the Claremont Hotel in Berkeley, CA for an ad-hoc two-week summer study. Fifty senior scientists from the major US ICF programs and accelerator laboratories participated, with program heads and Nobel laureates also attending. In the closing address, Dr. C. Martin Stickley, then Director of US-ERDA's Office of Inertial Fusion, announced the conclusion was "no showstoppers" on the road to fusion energy.
The two beam
Argus laser is completed at LLNL and experiments involving more advanced laser-target interactions commence.
Based on the continued success of the PLT, the DOE selects a larger Princeton design for further development. Initially designed simply to test a commercial-sized tokamak, the DOE team instead gives them the explicit goal of running on a deuterium-tritium fuel as opposed to test fuels like hydrogen or deuterium. The project is given the name
Tokamak Fusion Test Reactor (TFTR).
1977
The 20 beam
Shiva laser at LLNL is completed, capable of delivering 10.2 kilojoules of infrared energy on target. At a price of $25 million and a size approaching that of a football field, the Shiva laser is the first of the "megalasers" at LLNL and brings the field of ICF research fully within the realm of "
big science".
The
JET project is given the go-ahead by the
EC, choosing the UK's center at Culham as its site.
1978
As PLT continues to set new records, Princeton is given additional funding to adapt TFTR with the explicit goal of reaching breakeven.
1979
LANL successfully demonstrates the radio frequency quadrupole accelerator (RFQ).
ANL and Hughes Research Laboratories demonstrate required ion source brightness with xenon beam at 1.5MeV.
The Foster Panel report to US-DoE's Energy Research and advisory board on ICF concludes that
heavy ion fusion (HIF) is the "conservative approach" to ICF. Listing HIF's advantages in his report, John Foster remarked: "...now that is kind of exciting." After DoE Office of Inertial Fusion completed review of programs, Director Gregory Canavan decides to accelerate the HIF effort.
1980s
1982
HIBALL study by German and US institutions,[17] Garching uses the high repetition rate of the RF accelerator driver to serve four reactor chambers and first-wall protection using liquid lithium inside the chamber cavity.
Tore Supra construction starts at
Cadarache, France. Its
superconducting magnets will permit it to generate a strong permanent toroidal magnetic field.[18]
JET, the largest operational magnetic confinement plasma physics experiment is completed on time and on budget. First plasmas achieved.
The
NOVETTE laser at LLNL comes on line and is used as a test bed for the next generation of ICF lasers, specifically the
NOVA laser.
1984
The huge 10 beam
NOVA laser at LLNL is completed and switches on in December. NOVA would ultimately produce a maximum of 120 kilojoules of infrared laser light during a nanosecond pulse in a 1989 experiment.
1985
National Academy of Sciences reviewed military ICF programs, noting HIF's major advantages clearly but averring that HIF was "supported primarily by other [than military] programs".[citation needed] The review of ICF by the National Academy of Sciences marked the trend with the observation: "The energy crisis is dormant for the time being." Energy becomes the sole purpose of heavy ion fusion.
The Japanese tokamak,
JT-60 completed. First plasmas achieved.
1988
The
T-15, Soviet tokamak with superconducting helium-cooled coils completed.
The Conceptual Design Activity for the International Thermonuclear Experimental Reactor (
ITER), the successor to
T-15,
TFTR,
JET and
JT-60, begins.[19] Participants include
EURATOM, Japan, the
Soviet Union and United States. It ended in 1990.
On March 23, two
Utah electrochemists,
Stanley Pons and
Martin Fleischmann, announced that they had achieved
cold fusion: fusion reactions which could occur at room temperatures. However, they made their announcements before any peer review of their work was performed, and no subsequent experiments by other researchers revealed any evidence of fusion.
The
START Tokamak fusion experiment begins in
Culham. The experiment would eventually achieve a record
beta (plasma pressure compared to magnetic field pressure) of 40% using a
neutral beam injector. It was the first design that adapted the conventional toroidal fusion experiments into a tighter spherical design.
The Engineering Design Activity for the
ITER starts with participants
EURATOM, Japan, Russia and United States. It ended in 2001.
The United States and the former republics of the Soviet Union cease nuclear weapons testing.
1993
The
TFTR tokamak at
Princeton (PPPL) experiments with a 50%
deuterium, 50%
tritium mix, eventually producing as much as 10 megawatts of power from a controlled fusion reaction.
1994
NIF Beamlet laser is completed and begins experiments validating the expected performance of NIF.
The USA declassifies information about indirectly driven (hohlraum) target design.
Comprehensive European-based study of HIF driver begins, centered at the Gesellschaft für Schwerionenforschung (GSI) and involving 14 laboratories, including USA and Russia. The Heavy Ion Driven Inertial Fusion (HIDIF) study will be completed in 1997.
1996
A record is reached at
Tore Supra: a plasma duration of two minutes with a current of almost 1 million amperes driven non-inductively by 2.3 MW of
lower hybrid frequency waves (i.e. 280 MJ of injected and extracted energy). This result was possible due to the actively cooled plasma-facing components installed in the machine.[22]
The
JET tokamak in the UK produces 16 MW of fusion power - this remains the world record for fusion power until 2022 when JET sets an even higher record. Four megawatts of
alpha particle self-heating was achieved.
LLNL study compared projected costs of power from ICF and other fusion approaches to the projected future costs of existing energy sources.
The
JT-60 tokamak in Japan produced a high performance reversed shear plasma with the equivalent fusion amplification factor of 1.25 - the current world record of
Q, fusion energy gain factor.
Results of European-based study of heavy ion driven fusion power system (HIDIF, GSI-98-06) incorporates telescoping beams of multiple isotopic species. This technique multiplies the 6-D phase space usable for the design of HIF drivers.
1999
The United States withdraws from the
ITER project.
Building construction for the immense 192-beam 500-terawatt
NIF project is completed and construction of laser beam-lines and target bay diagnostics commences, expecting to take its first full system shot in 2010.
Negotiations on the Joint Implementation of
ITER begin between Canada, countries represented by the
European Union, Japan and Russia.
2002
Claims and counter-claims are published regarding
bubble fusion, in which a table-top apparatus was reported as producing small-scale fusion in a liquid undergoing
acoustic cavitation. Like cold fusion (see 1989), it is later dismissed.
The United States drops its own ITER-scale tokamak project,
FIRE, recognising an inability to match EU progress.[23]
2005
Following final negotiations between the EU and Japan,
ITER chooses
Cadarache over
Rokkasho for the site of the reactor. In concession, Japan is able to host the related materials research facility and granted rights to fill 20% of the project's research posts while providing 10% of the funding.
The
NIF fires its first bundle of eight beams achieving the highest ever energy laser pulse of 152.8 kJ (infrared).
2006
China's
EAST test reactor is completed, the first tokamak experiment to use superconducting magnets to generate both the toroidal and poloidal fields.
HIF-2010 Symposium in Darmstadt, Germany. Robert J Burke presented on Single Pass (Heavy Ion Fusion) HIF and Charles Helsley made a presentation on the commercialization of HIF within the decade.
2011
May 23–26, Workshop for Accelerators for Heavy Ion Fusion at Lawrence Berkeley National Laboratory, presentation by Robert J. Burke on "Single Pass Heavy Ion Fusion". The Accelerator Working Group publishes recommendations supporting moving RF accelerator driven HIF toward commercialization.[citation needed]
2012
Stephen Slutz & Roger Vesey of Sandia National Labs publish a paper in Physical Review Letters presenting a computer simulation of the
MagLIF concept showing it can produce high gain. According to the simulation, a 70 Mega Amp Z-pinch facility in combination with a Laser may be able to produce a spectacular energy return of 1000 times the expended energy. A 60 MA facility would produce a 100x yield.[24]
In August Robert J. Burke presents updates to the
SPRFDHIF process[25] and Charles Helsley presents the Economics of SPRFD[26] at the 19th International HIF Symposium at
Berkeley, California. Industry was there in support of ion generation for SPRFD. The Fusion Power Corporation SPRFD patent is granted in Russia.
2013
China's
EAST tokamak test reactor achieves a record confinement time of 30 seconds for plasma in the
high-confinement mode (H-mode), thanks to improvements in heat dispersal from tokamak walls. This is an improvement of an order of magnitude with respect to state-of-the-art reactors.[27]
US Scientists at
NIF successfully generate more energy from fusion reactions than the energy absorbed by the nuclear fuel.[28]
Phoenix Nuclear Labs announces the sale of a high-yield neutron generator that could sustain 5×1011deuterium fusion reactions per second over a 24-hour period.[29]
On 9 October 2014, fusion research bodies from European Union member states and Switzerland signed an agreement to cement European collaboration on fusion research and EUROfusion, the European Consortium for the Development of Fusion Energy, was born.[30]
2015
Germany conducts the first plasma discharge in
Wendelstein 7-X, a large-scale stellarator capable of steady-state plasma confinement under fusion conditions.[31]
In August,
MIT announces the
ARC fusion reactor, a compact tokamak using
rare-earth barium-copper oxide (REBCO) superconducting tapes to produce high-magnetic field coils that it claims produce comparable magnetic field strength in a smaller configuration than other designs.[33]
2016
The Wendelstein 7-X produces the device's first hydrogen plasma.[34]
2017
China's
EAST tokamak test reactor achieves a stable 101.2-second steady-state high confinement plasma, setting a world record in long-pulse H-mode operation on the night of July 3.[35]
Helion Energy's fifth-generation plasma machine goes into operation, seeking to achieve plasma density of 20 Tesla and fusion temperatures.[36]
UK company
Tokamak Energy's ST40 fusion reactor generates first plasma.[37]
MIT scientists formulate a theoretical means to remove the excess heat from compact nuclear fusion reactors via larger and longer
divertors.[42]
General Fusion begins developing a 70% scale demo system to be completed around 2023.[36]
TAE Technologies announces its reactor has reached a high temperature of nearly 20 million°C.[43]
The Fusion Industry Association founded as an initiative in 2018, is the unified voice of the fusion industry, working to transform the energy system with commercially viable fusion power.[44]
2019
The United Kingdom announces a planned £200-million (US$248-million) investment to produce a design for the
Spherical Tokamak for Energy Production (STEP) fusion facility around 2040.[45][46]
2020s
2020
Assembly of
ITER, which has been under construction for years, commences.[47]
The Chinese experimental
nuclear fusion reactor
HL-2M is turned on for the first time, achieving its first plasma discharge.[48]
2021
Record China's
EAST tokamak sets a new world record for superheated plasma, sustaining a temperature of 120 million degrees Celsius for 101 seconds and a peak of 160 million degrees Celsius for 20 seconds.[49]
Record The
National Ignition Facility achieves generating 70% of the input energy, necessary to sustain fusion, from
inertial confinementfusion energy, an 8x improvement over previous experiments in spring 2021 and a 25x increase over the yields achieved in 2018.[50]
The first Fusion Industry Association report was published - "The global fusion industry in 2021"[51]
Record China's
Experimental Advanced Superconducting Tokamak (EAST), a nuclear fusion reactor research facility, sustained plasma at 70 million degrees Celsius for as long as 1,056 seconds (17 minutes, 36 seconds), achieving the new world record for sustained high temperatures (fusion energy however requires i.a. temperatures over 150 million °C).[52][53][54]
2022
Record The
Joint European Torus in Oxford, UK, reports 59 megajoules produced with nuclear fusion over five seconds (11 megawatts of power), more than double the previous record of 1997.[55][56]
Record United States researchers at
Lawrence Livermore National Laboratory National Ignition Facility (NIF) in California has recorded the first case of ignition on August 8, 2021. Producing an energy yield of 0.72, of laser beam input to fusion output.[57][58]
Record Building on the achievement in August 2022, American researchers at
Lawrence Livermore National Laboratory National Ignition Facility (NIF) in California recorded the first ever net energy production with nuclear fusion, producing more fusion energy than laser beam put in. Laser efficiency was in the order of 1%.[59]
2023
Record On February 15, 2023,
Wendelstein 7-X reached a new milestone: Power plasma with gigajoule energy turnover generated for eight minutes.[60]
JT-60SA achieves first plasma in October, making it the largest operational superconducting tokamak in the world.[61]
2024
The Korea Superconducting Tokamak Advanced Research (
KSTAR) achieved the new record of 102-sec-long operation (Integrated RMP control for ELM-less H-mode with a notable advancement on the favorable control the error field,[62] Tungsten divertor) with the achieved duration of 48 seconds at the high-temperature of about 100 million degrees Celsius in February 2024, after the last record of 45-sec-long operation (ELM-less H-mode (FIRE mode[63]), Carbon-based divertor, 2022). See
"핵융합 플라스마 장기간 운전기술 확보 청신호, 보도자료, KSTAR연구본부" (in Korean). 20 March 2024. and
"[공식발표] 한국 인공태양 KSTAR 또 해냈다! "1억도○○ 초?"". YouTube (in Korean). (21 March 2024).
^Nimtz, G.; Clegg, B. (12 August 2009). Greenberger, D.; Hentschel, K.; Weinert, F. (eds.). Compendium of Quantum Physics. Springer. pp. 799–802.
ISBN978-3-540-70622-9.
^...the first money to be allocated [to controlled nuclear research] happened to be for Tuck, and was diverted from Project Lincoln, in the Hood Laboratory. The coincidence of names prompted the well-known cover name "Project Sherwood". James L. Tuck,
"Curriculum Vita and Autobiography", declassified document from Los Alamos National Laboratory (1974), reproduced with permission.
Archived 9 February 2012.
^"Lecture of I.V. Kurchatov at Harwell", from the address of I.V. Kurchatov: "On the possibility of producing thermonuclear reactions in a gas discharge" at Harwell on 25 April 1956.
Archived 20 July 2015.
^"Hans Bethe". Hans Bethe - Biographical. Nobel Prize.org. Retrieved 11 March 2016.
^...Gesellschaft für Schwerionenforschung; Institut für Plasmaphysik, Garching; Kernforschungszentrum Karlsruhe, University of Wisconsin, Madison; Max-Planck-Institut für Quantenoptik
^"Tore Supra". www-drfc.cea.fr. Archived from
the original on 15 November 2012. Retrieved 15 January 2022.
^那珂研究所 (1991). Annual report of the Naka Fusion Research Establishment for the period of April 1, 1990 to March 31, 1991 (Report) (in Japanese). 日本原子力研究開発機構.
doi:
10.11484/jaeri-m-91-159.
^Burke, Robert (1 January 2014). "The Single Pass RF Driver: Final beam compression". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 733: 158–167.
Bibcode:
2014NIMPA.733..158B.
doi:
10.1016/j.nima.2013.05.080.
^Helsley, Charles E.; Burke, Robert J. (January 2014). "Economic viability of large-scale fusion systems". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 733: 51–56.
Bibcode:
2014NIMPA.733...51H.
doi:
10.1016/j.nima.2013.05.095.
^ S.M.Yang et al., Tailoring tokamak error fields to control plasma instabilities and transport, Nature Communications,
10 February 2024,
https://doi.org/10.1038/s41467-024-45454-1
^ H.Han et al., A sustained high-temperature fusion plasma regime facilitated by fast ions, Nature 609, 8 September 2022, 269-275. doi:10.1038/s41586-022-05008-1.
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