Skip to main content

Thank you for visiting nature.com. You are using a browser version with limited support for CSS. To obtain the best experience, we recommend you use a more up to date browser (or turn off compatibility mode in Internet Explorer). In the meantime, to ensure continued support, we are displaying the site without styles and JavaScript.

Achieving a long-lived high-beta plasma state by energetic beam injection

Abstract

Developing a stable plasma state with high-beta (ratio of plasma to magnetic pressures) is of critical importance for an economic magnetic fusion reactor. At the forefront of this endeavour is the field-reversed configuration. Here we demonstrate the kinetic stabilizing effect of fast ions on a disruptive magneto-hydrodynamic instability, known as a tilt mode, which poses a central obstacle to further field-reversed configuration development, by energetic beam injection. This technique, combined with the synergistic effect of active plasma boundary control, enables a fully stable ultra-high-beta (approaching 100%) plasma with a long lifetime.

Introduction

Nuclear fusion potentially offers a clean, environment-friendly and intrinsically safe energy source with an abundant fuel supply. A promising approach to harnessing fusion power utilizes magnetic fields to confine a plasma with sufficient density and energy confinement time to achieve sustained thermonuclear temperatures, exceeding 100 million degrees Celsius for a fusion reactor fuelled by the hydrogen isotopes: deuterium (D) and tritium (T)1,2. The most advanced approach for magnetic confinement fusion is a doughnut-shaped confinement system known as a Tokamak3, as evidenced by a joint international effort in building a major next-step facility, international thermonuclear experimental reactor (ITER; http://www.iter.org), to demonstrate scientific viability and some essential technologies for a fusion reactor. Anticipating scientific and technological successes of ITER, economic viability, ease of maintenance and safety should advance to the forefront of fusion energy development towards ultimate commercial use.

The field-reversed configuration (FRC) is a simple compact toroid (CT) magnetic confinement system, that is, one without toroidal coils linking the plasma4,5, and thus with predominantly poloidal fields. The attractions of such a configuration for a potential fusion reactor are its simple, linear geometry for ease of construction and maintenance, as well as a natural, unrestricted divertor configuration for facilitating energy extraction and fusion ash removal. The FRC is a diamagnetic entity with current flowing across the magnetic field lines. Having no appreciable toroidal magnetic field greatly reduces the threat of dangerous disruptive events associated with massive magnetic energy and runaway electrons6, a great challenge facing fusion reactors. In addition, of all magnetic confinement systems, the FRC exhibits the highest β, defined as the ratio of the plasma pressure to the magnetic energy density of the externally supplied magnetic fields, approaching 100%, thus allowing for efficient use of magnet hardware. The high-β property also allows the use of advanced fusion fuels7,8. These features, coupled with its unique linear exhaust capability, also make the FRC a highly attractive candidate vehicle for deep-space explorations9.

In the following, we report on a kinetic effect to stabilize a highly disruptive instability for an FRC, known as a tilt mode, provided by fast ions from energetic beam injection. The tilt mode is manifested as a spontaneous relaxation event marked by the abrupt ejection of a fraction of plasma from the confined region. The instability can be prevented altogether at a sufficient fast particle concentration. Another new finding is that active wall conditioning with titanium or lithium gettering to control edge neutrals and impurities is imperative for maintaining FRC stability by preventing density rise during the discharge. Such a stabilizing effect from fast particles, combined with the synergistic effect of the active boundary control, enables achievement of a fully-stable FRC scenario with a long lifetime.

Results

C-2 CT-merging FRC experiment

Spectacular progress has been made on both physics and technology fronts of FRC development in the C-2 CT-merging FRC experiment (Fig. 1)10,11,12,13, an effort entirely funded by private resources. It has recently achieved a long-lived FRC regime, with a marked improvement in confinement over one order of magnitude, departing from the predictions based on the scaling law in the previous experiments14.

Figure 1: Schematic of C-2 merging CT facility.
figure1

C-2 system consists of a centre stainless-steel confinement vessel, two theta-pinch formation sections on opposite sides of the confinement chamber, and two divertors at both ends, with total axial span of 20 m. There are eight neutral beams, three on each side of the confinement chamber and two on top of the confinement chamber for current drive and heating. Two plasma guns are located near the axial ends of the machine for active control of edge plasma.

C-2 has adopted a collision-merging FRC formation scheme15,16,17 by colliding two high-β CTs at a supersonic speed, each formed by a conventional theta-pinch10,11, producing high-temperature FRCs with radius rs0.35 m, length , density ne5 × 1019 m−3, total temperature Tt=Ti+Te up to 1 keV, external magnetic field, Be0.1 T, plasma current Ip 0.5 MA, , as expected for an FRC. The merged FRCs are centred in a metallic cylindrical confinement chamber of radius 0.7 m and length 5 m with strong magnetic mirrors (mirror ratio 3) at the cone-shaped ends of the chamber. The ultimate goal of C-2 is to achieve fusion-relevant FRC plasmas and explore their sustainment by neutral beam injection (NBI). The 20 keV hydrogen beams are injected tangentially into the confinement chamber with an impact parameter of 0.2 m before the FRC merging process. In view of the low internal magnetic field, the orbits of fast ions generated by NBI extend well outside the magnetic separatrix. This makes it essential to limit the edge neutral density to minimize fast-ion losses via charge exchange with cold neutrals18. Towards this end, an extensive effort of wall conditioning, using titanium gettering and advanced lithium-coating techniques, reduced both the neutral concentration in the edge plasma (well below 0.1%) and impurity radiation.

In addition, we have demonstrated an active means of improving the stability and confinement property of the merged FRC as a suitable target plasma for NBI by applying line-tying and boundary-plasma biasing with plasma guns at the end divertors12,13. The former provides a restoring force that facilitates the centring of the plasma and reduces the off-centre ‘wobble’, while the latter produces an inward electric field Er with the Er × Bz drift opposing the ion diamagnetic drift Bz × p, thus reducing bulk plasma rotation. This proves effective at suppressing the magneto-hydrodynamic (MHD) instability with azimuthal mode number l=2 (the disturbance has the factor eilθ where θ is the azimuth angle), which is driven by centrifugal forces developed from plasma rotation4,5. The end-electric biasing is also effective at suppressing edge fluctuations, thus improving confinement.

Achievement of long-lived FRCs

Coupling these active boundary control techniques with NBI, we have achieved long-lived FRCs, with the lifetime approaching 5 ms, far beyond the conventional theta-pinch-formed FRCs4,14,19,20, as shown in Fig. 2. Here, the lifetime is defined as the time interval before the plasma radius falls to zero. Without NBI FRCs quickly disrupt with a much shorter lifetime and exhibit large shot-to-shot variations. Actually, the particular time trace shown in the figure for the case without NBI is averaged over a large number of discharges under the same operating conditions. This achievement clearly demonstrates NBI as an essential component for attaining FRC stability, against the potential l=1 tilt mode21, which has cast a great shadow over FRC development to date4,5. In common stability parlance the tilt is the lowest-order kink mode, but, unlike rotational modes, it is largely an internal disturbance in elongated FRCs with primarily an axial shift. The tilt is predicted to be the most dangerous instability of all by MHD theory because its ideal growth time is extremely short with 1/γmhd5 μs for typical C-2 FRCs, which can lead to the destruction of FRC topology. Here, is the predicted growth rate of the ideal tilt instability with being the FRC length, being the Alfven speed based on the external magnetic field and the average density (mi is the ion mass and μ0 is the free-space permeability). Despite this fast ‘self-destruct’ rate, past FRCs usually survived a few dozen times longer than 1/γmhd (ref. 5), commonly ascribed to the highly kinetic nature of FRCs22,23,24,25,26 and two-fluid effects27,28,29; other stabilizing influences may have contributed in past experiments as well: sheared flow30; small toroidal fields20,31,32,33; and rotating magnetic fields34,35.

Figure 2: Demonstration of long-lived FRCs with a lifetime far beyond conventional theta-pinch formed FRCs by neutral beam injection.
figure2

Shown here are the time histories of the normalized excluded flux radius, which approximates the confined plasma radius, rΔφrs, for a series of consecutive discharges obtained in C-2 with neutral beams, along with that averaged over a number of similar discharges without neutral beams. Also shown is a typical FRC obtained from the translation, confinement and sustainment (TCS) FRC experiment19,20, one of the previous longest-lived FRCs. (Errors for the magnetic measurements are <5%.).

Stabilizing effects from neutral beam injection

The highly kinetic property causes the ion and magnetic disturbances to get out of phase, which can stabilize or at least greatly reduce the growth rate22,36. NBI creates a large-orbit ion population, which potentially contributes to the kinetic effects, thus providing additional stability, but it has never been demonstrated before. We have employed the hybrid kinetic MHD (HKMHD) model in the 3D NIMROD code37 to examine possible stabilizing effects of NBI to the l=1 tilt mode. In these simulations, the fast ion component (arising from NBI) is represented as a collisionless species using a particle-in-cell technique, with the bulk plasma being treated as an MHD fluid. The fast particle motion is coupled to the background fluid only through its influence on the magnetic field24. Thus, the thermal fluid equation of motion and resistive Ohm’s law remain the same but the Ampere’s law is adjusted as , where J is the thermal fluid current (ions+electrons), Jb is the current driven by the fast particles from neutral beams, B is the magnetic field and μ0 is the permeability of free space. For simulations with C-2 like parameters, the code predicts that without NBI the l=1 tilt mode grows and quickly disrupts the configuration within a few Alfvén times, as shown in Fig. 3. In contrast, the growth of the simulated tilt mode can be suppressed at a ratio of the fast-particle to thermal-ion density nb/ni7%, which is largely consistent with the experimental observations. For typical equilibrium FRCs after the merging formation process in C-2, the plasma contains 1019 ions and 1018 fast particles from NBI, hence, the fast particle concentration nb/ni10%. Note, however, that the fast particle pressure is of similar order of magnitude to the thermal plasma pressure. This implies that high-energy beams will be needed for a reactor because of much higher plasma pressure. This awaits further investigation by taking into account contribution from fusion products such as alpha particles.

Figure 3: Stabilizing effects from fast ions arising from NBI.
figure3

The growth of the kinetic energy of the tilt mode predicted by the HKMHD/NIMROD code for a typical C-2 equilibrium with a fast particle concentration nb/ni=7% (NBI), in comparison with the case with nb/ni=0 (no NBI).

HKMHD/NIMROD modelling shows that the tilt mode leads to an axial shift with a significant (l=1) perturbation to the radial magnetic field Br at the FRC ends, while the beam current maintains a dominant azimuthal component to Jb in this region owing to large-orbit kinetic effects. This leads to an effective axial <Jb,θ × Br> restoring force, hence providing a stabilizing effect on the tilt mode, as originally demonstrated numerically by Barnes and Milroy24. It is worth noting that, for the calculations shown in Fig. 3, the l=1 mode is unstable for the initial beam parameters, but as the mode starts to grow it causes the beam to spread axially. That is the beam adjusts itself due to the perturbation, and after this adjustment the beam is more stabilizing, and the mode then decays.

Another important finding for the achievement of the stable long-lived FRC scenario is the need for advanced wall conditioning with titanium gettering or lithium coating. In addition to improving NBI coupling to the FRC, as aforementioned, this also reduces recycling and impurity production resulting from plasma–wall interactions to avoid an unwanted growth in the density and consequent rise in S* for maintaining stability. where is the ion skin depth (a measure of the ion orbit size at high-β); it measures the degree to which the plasma reacts like a fluid (high S*) or an orbit-dominated (low S*) object. An uncontrolled rise in plasma density tends to cause onset of a spontaneous transition midway through the discharge, which appears to be driven by the tilt mode (as discussed later), degrading the performance, even prematurely terminating the configuration. As shown in Fig. 4, the transition event is manifested as an abrupt drop in the excluded flux radius rΔφ. The excluded flux radius is rΔφ≡(Δφ/πBe)1/2, where Δφ is the excluded magnetic flux as measured by a probe array arranged along the length of the confinement chamber. The rΔφ in the figure is the maximum value, which is always near the axial midplane (z=0). It represents the radius of the confined plasma on the closed magnetic field lines, approximating the magnetic separatrix radius, rΔφrs. The change in rΔφ has a major implication, as the poloidal flux φp is strongly dependent on rΔφ. Recall that φp is generated entirely by the cross-field plasma current. In contrast to other magnetic confinement systems, in FRCs the poloidal flux typically decays on the resistive timescale, closely inter-coupled to the cross-field transport rate. Thus, the abrupt (<0.1 ms) drop of rΔφ during the transition marks a magnetic-reconnection event that annihilates a fraction of the poloidal flux. Simultaneous with it is a crash in the average density (Fig. 4b) and a rapid increase in the apparent plasma length (Fig. 4e). An integral part of this major restructuring is the ejection of a fraction of the plasma, as witnessed by the radiation bursts at the FRC ends immediately following the transition (Fig. 4c,d), detected by the bolometers located at z=±1 m from the midplane. The time delay is about 80 μs between the onset of the transition, as manifested by a spontaneous decrease in rΔφ, and the bursts of radiations at the FRC ends, commensurate with a jet velocity of 12 km s−1. This is reminiscent of the ejecta from astrophysical jets and coronal mass ejections38,39,40,41. Incidentally, relaxation has also been observed during dynamic FRC formation processes10,11,19, suggesting the tendency towards a preferred plasma state in these high-β systems, just as is well known in some low-β laboratory plasmas42,43,44,45,46,47.

Figure 4: Spontaneous transition during long-lived FRCs with NBI.
figure4

The time traces of a series of discharges with and without transition. Data shown are the excluded flux radius, rΔφ, the line averaged electron density, , at the midplane of FRC, z=0, the radiated power at z=±1 m from the midplane, Prad,end, and the length of FRC, . Yellow shading indicates the time when the transition occurs for shots 24014, 24049 and 24076. (The lowest limit for the line-integrated density measurement is 0.3 × 1019 m−2, and the absolute responsivity of bolometers varies between −30 and +50%, dependent on the photon energy.)

Of particular importance is that the internal tilt mode usually leads to reconnection and annihilation of internal magnetic fields and hence termination of FRC. With application of neutral beam injection, the plasma usually relaxes into another FRC equilibrium, albeit with a lower internal magnetic flux, for typical FRC conditions in C-2. Moreover, this can be completely avoided while leveraging the synergistic effect from active boundary control, as demonstrated in Fig. 4. The key parameters affecting tilt instability are S* and the elongation of the separatrix (ref. 5). Figure 5 shows the trajectory of S*/E in the long-pulse discharges shown in the previous figure discussed above, where rs is approximated by rΔφ and is estimated from excluded-flux-array measurements. We can see that, for the cases with transition, as the FRC elongation, E, dwindles (shots 24014, 24049), the FRC proceeds towards a higher S*/E value, finally approaching the instability boundary with S*/E 3, as expected from the tilt theory. It is worth noting that as the elongation increases on relaxation, the plasma rebounds from the instability boundary, as predicted by tilt stability theory and verified by extensive modelling5. It then restructures into a new state, staying safely away from the transition. No other instabilities that have been identified for FRCs until now can explain these observations.

Figure 5: Progression of FRC towards tilt instability boundary S*/E 3.
figure5

The results are obtained from the three beam-driven long-pulse discharges shown in the previous figure. The solid and open symbols represent the data points before and after transition, respectively, with the arrows indicating time evolution of the discharges. The error bars represent the s.d. of the measurements.

The physics process of the relaxation driven by tilt is illustrated by HKMHD/NIMROD modelling, as shown in Fig. 6. As the FRC elongation E shrinks, the pressure profile peaks near the midplane (Fig. 6a), and the FRC becomes unstable to the tilt mode. The tilt mode leads to a significant perturbation in the plasma pressure profile, much larger than the magnetic perturbation. Clearly, the pressure profile exhibits an axial displacement, as manifested by the shifts in the bright spots in Fig. 6b. The code predicts that the beam current perturbation is out of phase with the plasma pressure perturbation. This, in turn, reduces the growth of the tilt mode, and the plasma enters a new stable and quiescent equilibrium state. In particular, the modelling shows that the pressure profile expands axially during the relaxation, leading to an increase in the elongation, E, to steer away from the instability cliff to reach the final relaxed state (Fig. 6c), in agreement with the experiments.

Figure 6: 3D HKMHD/NIMROD reproduces the FRC transition.
figure6

Contours of plasma pressure in an FRC with a relatively small fast particle concentration from NBI, obtained from HKMHD/NIMROD calculations. (a) In the equilibrium phase before the development of the tilt mode. (b) During the tilt mode at maximum perturbation. (c) In the new quiescent state after tilt perturbation decays away.

Discussion

A central obstacle to FRC development is its stability to the MHD instabilities with low azimuthal mode numbers, that is, l=1 tilt mode and l=2 rotational mode4. The stability of the l=2 rotational mode has been achieved by applying various control techniques, for example, external static fields4, rotating magnetic fields34 and the plasma gun12,13. However, active stabilization of the most dangerous l=1 tilt mode has not been demonstrated before this work. The tilt mode leads to tearing and annihilation/reconnection of the internal magnetic flux surface, and thus the loss of FRC magnetic configuration. We have demonstrated the stabilizing effect of fast ions by NBI, achieving a stable, high-β plasma state with a lifetime of about 5 ms. This achievement was enabled by the injection of energetic particles from NBI in concert with active plasma boundary control. These advances enhance the prospect of an economic fusion reactor with an extremely high β and simple geometry, thus providing a compelling additional platform for the development of economic fusion energy.

Methods

The C-2 device

The C-2 is an FRC facility that was designed to demonstrate FRC sustainment with the neutral beam injection for heating and current drive. The C-2 device consists of a central confinement vessel, interposed between two CT formation sections, and two divertor chambers at each end to control neutrals and impurities. Typical C-2 equilibrium FRC parameters are as follows: separatrix radius rs 0.4 m, separatrix length , external magnetic field Be 0.1 T, average density ne 5 × 1019 m−3, total temperature Tt=Ti+Te up to 1 keV and plasma current Ip 0.5 MA. The C-2 is equipped with eight neutral beams distributed around the azimuth and along the central confinement vessel of the machine, and two plasma-guns mounted coaxially in each divertor.

NB injection

On the C-2 device NB injection offers a most principal means for FRC plasma heating, current drive and stabilization. Six NBs (20 keV, Hydrogen, 0.7 MW per unit) with total 4 MW power are routinely injected perpendicular to the confinement chamber and aimed tangentially in the FRC current direction (co-injection), with an impact parameter of 0.2 m. The C-2 FRC parameters are suitable for NB capture (Monte-Carlo simulations indicate that shine-through and first orbit losses less than 10%) and for fast ion confinement (slowing down time FRC lifetime). The fast ions, created by charge exchange, trace out large-scale betatron orbits that contribute to the plasma current and build up a fast-ion population with pressure eventually comparable to the thermal pressure.

Plasma gun

The plasma guns on C-2 are used to produce and direct plasma flows at high-energy densities. These plasma guns generate a warm (electrons Te 30–50 eV, ions Ti 100 eV), tenuous (ne <1019 m−3) and annular (0.11 m inner diameter and 0.13 m outer diameter) plasma stream for about 6 ms. The typical anode-to-cathode voltage difference is 500 V, and the gun arc-current is 10 kA. The gun magnet provides an axial magnetic field 0.5 T. The plasma guns perform multiple functions (1) to create an inward radial electric field in the scrape off layer (SOL) (important for stabilizing n=2 rotational mode), (2) to establish electromagnetic shear in the SOL (effective to suppress local fluctuations) and (3) to tightly centre the plasma (less n=1 wobble motion) via line-tying to the gun electrodes.

Additional information

How to cite this article: Guo, H. Y. et al. Achieving a long-lived high-beta plasma state by energetic beam injection. Nat. Commun. 6:6897 doi: 10.1038/ncomms7897 (2015).

References

  1. 1

    Hawryluk, R. J. Results from deuterium-tritium tokamak confinement experiments. Rev. Mod. Phys. 70, 537–587 (1998).

    CAS  ADS  Article  Google Scholar 

  2. 2

    Keilhacker, M. et al. High fusion performance from deuterium-tritium plasmas in JET. Nucl. Fusion 39, 209–234 (1999).

    CAS  ADS  Article  Google Scholar 

  3. 3

    Wesson, J. Tokamaks 4th edn Oxford University Press (2011).

  4. 4

    Tuszewski, M. Field reversed configurations. Nucl. Fusion 28, 2033–2092 (1988).

    CAS  Article  Google Scholar 

  5. 5

    Steinhauer, L. C. Review of field-reversed configurations. Phys. Plasmas 18, 070501 (2011).

    ADS  Article  Google Scholar 

  6. 6

    Loarte, A. et al. Power and particle control. Nucl. Fusion 47, S203–S263 (2007).

    CAS  Article  Google Scholar 

  7. 7

    Berk, H. L. et al. Plasma current sustained by fusion charged particles in a field reversed configuration. Phys. Fluids 30, 3548–3565 (1987).

    CAS  ADS  Article  Google Scholar 

  8. 8

    Rostoker, N. et al. Colliding beam fusion reactor. Science 278, 1419–1422 (1997).

    CAS  ADS  Article  Google Scholar 

  9. 9

    Czysz, P. A. et al. Future Spacecraft Propulsion Systems 2nd edn Praxis Publishing Ltd (2009).

  10. 10

    Binderbauer, M. W. et al. Dynamic formation of a hot field reversed configuration with improved confinement by supersonic merging of two colliding high-β compact toroids. Phys. Rev. Lett. 105, 045003 (2010).

    CAS  ADS  Article  Google Scholar 

  11. 11

    Guo, H. Y. et al. Formation of a long-lived hot field reversed configuration by dynamically merging two colliding high-β compact toroids. Phys. Plasmas 18, 056110 (2011).

    ADS  Article  Google Scholar 

  12. 12

    Tuszewski, M. et al. Field reversed configuration confinement enhancement through edge biasing and neutral beam injection. Phys. Rev. Lett. 108, 255008 (2012).

    CAS  ADS  Article  Google Scholar 

  13. 13

    Tuszewski, M. et al. A new high performance field reversed configuration operating regime in the C-2 device. Phys. Plasmas 19, 056108 (2012).

    ADS  Article  Google Scholar 

  14. 14

    Hoffman, A. L. et al. Field reversed configuration lifetime scaling based on measurements from the large s experiment. Nucl. Fusion 33, 27–38 (1993).

    CAS  ADS  Article  Google Scholar 

  15. 15

    Wells, D. R. Injection and trapping of plasma vortex structures. Phys. Fluids 9, 1010–1021 (1966).

    ADS  Article  Google Scholar 

  16. 16

    Wells, D. R. et al. High-temperature, high-density plasma production by vortex-ring compression. Phys. Rev. Lett. 41, 166–170 (1978).

    CAS  ADS  Article  Google Scholar 

  17. 17

    Votroubek, G., Slough, J., Andreason, S. & Pihl, C. Formation of a stable field reversed configuration through merging. J. Fusion Energy 27, 123–127 (2008).

    CAS  Article  Google Scholar 

  18. 18

    Stangeby, P. C. The Plasma Boundary of Magnetic Fusion Devices IOP (2000).

  19. 19

    Guo, H. Y. et al. Flux conversion and evidence of relaxation in a high-β plasma formed by high-speed injection into a mirror confinement structure. Phys. Rev. Lett. 92, 245001 (2004).

    CAS  ADS  Article  Google Scholar 

  20. 20

    Guo, H. Y. et al. Observation of improved confinement in a high-β self-organized shperical-torus-like field-reversed configuration. Phys. Rev. Lett. 95, 175001 (2005).

    CAS  ADS  Article  Google Scholar 

  21. 21

    Rosenbluth, M. N. et al. MHD stability of spheromak. Nucl. Fusion 19, 489–498 (1979).

    ADS  Article  Google Scholar 

  22. 22

    Belova, E. V. et al. Kinetic effects on the stability properties of field-reversed configurations. I. Linear. Phys. Plasmas 10, 2361–2371 (2003).

    CAS  ADS  MathSciNet  Article  Google Scholar 

  23. 23

    Steinhauer, L. C. et al. Gyroviscous stability theory with application to the internal tilt mode of a field reversed configuration. Phys. Fluids B 2, 2422–2430 (1990).

    CAS  ADS  Article  Google Scholar 

  24. 24

    Barnes, D. C. et al. Stabilization of the field-reversed configuration (FRC) tilt instability with energetic ion beams. Phys. Fluids B 3, 2609–2616 (1991).

    CAS  ADS  Article  Google Scholar 

  25. 25

    Belova, E. V. et al. Kinetic effects on the stability properties of field-reversed configurations. II. Nonlinear evolution. Phys. Plasmas 11, 2523–2531 (2004).

    CAS  ADS  MathSciNet  Article  Google Scholar 

  26. 26

    Belova, E. V. et al. Advances in the numerical modeling of field-reversed configurations. Phys. Plasmas 13, 056115 (2006).

    ADS  Article  Google Scholar 

  27. 27

    Ishida, A. et al. Variational formulation for a multifluid flowing plasma with application to the internal tilt mode of a fieldreversed configuration. Phys. Fluids 31, 3014–3034 (1988).

    ADS  Article  Google Scholar 

  28. 28

    Mahajan, S. M. et al. Double Curl Beltrami flow: diamagnetic structures. Phys. Rev. Lett. 30, 4863–4866 (1998).

    ADS  Article  Google Scholar 

  29. 29

    Barnes, D. C. Stability of long field-reversed configurations. Phys. Plasmas 9, 560–568 (2002).

    CAS  ADS  MathSciNet  Article  Google Scholar 

  30. 30

    Ono, Y. et al. Spontaneous and artificial generation of sheared-flow in oblate FRCs in TS-3 and 4 FRC experiments. Nucl. Fusion 43, 649–654 (2003).

    CAS  ADS  Article  Google Scholar 

  31. 31

    Guo, H. Y. et al. Evidence of relaxation and spontaneous rransition to a high-confinement state in high-beta steady-state plasmas sustained by rotating magnetic fields. Phys. Rev. Lett. 97, 235002 (2006).

    CAS  ADS  Article  Google Scholar 

  32. 32

    Milroy, R. D. et al. Toroidal field stabilization of the rotational instability in field-reversed configurations. Phys. Plasmas 15, 022508 (2008).

    ADS  Article  Google Scholar 

  33. 33

    Yang, X. et al. Effect of toroidal magnetic field on n=1 mode stability in rotamak plasmas. Phys. Plasmas 18, 080708 (2011).

    ADS  Article  Google Scholar 

  34. 34

    Guo, H. Y. et al. Stabilization of interchange modes by rotating magnetic fields. Phys. Rev. Lett. 94, 185001 (2005).

    CAS  ADS  Article  Google Scholar 

  35. 35

    Yang, X. et al. Suppression of n=1 tilt instability by magnetic shaping coils in rotamak plasmas. Phys. Rev. Lett. 102, 255004 (2009).

    CAS  ADS  Article  Google Scholar 

  36. 36

    Belova, E. V. et al. Numerical study of tilt stability of prolate field-reversed configurations. Phys. Plasmas 7, 4996–5006 (2000).

    CAS  ADS  Article  Google Scholar 

  37. 37

    Sovinec, C. R. et al. Nonlinear magnetohydrodynamics simulation using high-order finite elements. J. Comput. Phys. 195, 355–386 (2004).

    ADS  Article  Google Scholar 

  38. 38

    Masuda, S. et al. A loop-top hard X-ray source in a compact solar flare as evidence for magnetic reconnection. Nature 371, 495–497 (1994).

    ADS  Article  Google Scholar 

  39. 39

    Maehara, H. et al. Superflares on solar-type stars. Nature 485, 478–481 (2012).

    CAS  ADS  Article  Google Scholar 

  40. 40

    Tajima, T. & Shibata, K. Plasma Astrophysics Addison-Wesley, Reading (1997).

  41. 41

    Kulsrud, R. M. Plasma Physics for Astrophysics Princeton Univ. Press (2005).

  42. 42

    Taylor, J. B. et al. Relaxation of toroidal plasma and generation of reverse magnetic fields. Phys. Rev. Lett. 33, 1139–1141 (1974).

    ADS  Article  Google Scholar 

  43. 43

    Yamada, M. et al. Investigation of magnetic reconnection during a sawtooth crash in a high temperature tokamak plasma. Phys. Plasmas 1, 3269–3276 (1994).

    CAS  ADS  Article  Google Scholar 

  44. 44

    Brown, M. R. Experimental studies of magnetic reconnection. Phys. Plasmas 6, 1717–1724 (1999).

    CAS  ADS  Article  Google Scholar 

  45. 45

    Bellan, P. M. Spheromaks Imperial Coll Press (2000).

  46. 46

    Intrator, T. P. et al. Experimental onset threshold and magnetic pressure pile-up for 3D reconnection. Nat. Phys. 5, 521–526 (2009).

    CAS  Article  Google Scholar 

  47. 47

    Moser, A. L. et al. Magnetic reconnection from a multiscale instability cascade. Nature 482, 379–381 (2012).

    CAS  ADS  Article  Google Scholar 

Download references

Acknowledgements

We thank for the support and contributions from the rest of the TAE team and collaborators. A debt of gratitude is also due to our shareholders for their continuous support.

Author information

Affiliations

Authors

Contributions

All authors contributed to all aspects of this work.

Corresponding author

Correspondence to H. Y. Guo.

Ethics declarations

Competing interests

The authors declare no competing financial interests.

Rights and permissions

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

Guo, H., Binderbauer, M., Tajima, T. et al. Achieving a long-lived high-beta plasma state by energetic beam injection. Nat Commun 6, 6897 (2015). https://doi.org/10.1038/ncomms7897

Download citation

Further reading

Comments

By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.

Search

Quick links

Nature Briefing

Sign up for the Nature Briefing newsletter — what matters in science, free to your inbox daily.

Get the most important science stories of the day, free in your inbox. Sign up for Nature Briefing