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May 2006

Volume 13, Issue 5, Articles (05xxxx)

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Neoclassical tearing modes and their control

R. J. La Haye

Phys. Plasmas 13, 055501 (2006); http://dx.doi.org/10.1063/1.2180747 (18 pages) | Cited 78 times

Online Publication Date: 11 May 2006

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A principal pressure limit in tokamaks is set by the onset of neoclassical tearing modes (NTMs), which are destabilized and maintained by helical perturbations to the pressure-gradient driven “bootstrap” current. The resulting magnetic islands break up the magnetic surfaces that confine the plasma. The NTM is linearly stable but nonlinearly unstable, and generally requires a “seed” to destabilize a metastable state. In the past decade, NTM physics has been studied and its effects identified as performance degrading in many tokamaks. The validation of NTM physics, suppressing the NTMs, and/or avoiding them altogether are areas of active study and considerable progress. Recent joint experiments give new insight into the underlying physics, seeding, and threshold scaling of NTMs. The physics scales toward increased NTM susceptibility in ITER, underlying the importance of both further study and development of control strategies. These strategies include regulation of “sawteeth” to reduce seeding, using static “bumpy” magnetic fields to interfere with the perturbed bootstrap current, and/or applying precisely located microwave power current drive at an island to stabilize (or avoid destabilization of) the NTM. Sustained stable operation without the highly deleterious m = 2, n = 1 island has been achieved at a pressure consistent with the no-wall n = 1 ideal kink limit, by using electron cyclotron current drive at the q = 2 rational surface, which is found by real-time accurate equilibrium reconstruction. This improved understanding of NTM physics and stabilization strategies will allow design of NTM control methods for future burning-plasma experiments like ITER.
Show PACS
52.35.Py Macroinstabilities (hydromagnetic, e.g., kink, fire-hose, mirror, ballooning, tearing, trapped-particle, flute, Rayleigh-Taylor, etc.)
52.55.Fa Tokamaks, spherical tokamaks
52.55.Wq Current drive; helicity injection
52.25.Fi Transport properties
52.35.Mw Nonlinear phenomena: waves, wave propagation, and other interactions (including parametric effects, mode coupling, ponderomotive effects, etc.)

Physics of zonal flows

K. Itoh, S.-I. Itoh, P. H. Diamond, T. S. Hahm, A. Fujisawa, G. R. Tynan, M. Yagi, and Y. Nagashima

Phys. Plasmas 13, 055502 (2006); http://dx.doi.org/10.1063/1.2178779 (11 pages) | Cited 74 times

Online Publication Date: 15 May 2006

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Zonal flows, which means azimuthally symmetric band-like shear flows, are ubiquitous phenomena in nature and the laboratory. It is now widely recognized that zonal flows are a key constituent in virtually all cases and regimes of drift wave turbulence, indeed, so much so that this classic problem is now frequently referred to as “drift wave-zonal flow turbulence.” In this review, new viewpoints and unifying concepts are presented, which facilitate understanding of zonal flow physics, via theory, computation and their confrontation with the results of laboratory experiment. Special emphasis is placed on identifying avenues for further progress.
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52.30.-q Plasma dynamics and flow
52.35.Kt Drift waves
52.35.Ra Plasma turbulence
52.25.Fi Transport properties
01.30.Rr Surveys and tutorial papers; resource letters

Plasma accelerators race to 10 GeV and beyond

T. Katsouleas

Phys. Plasmas 13, 055503 (2006); http://dx.doi.org/10.1063/1.2198172 (7 pages) | Cited 8 times

Online Publication Date: 22 May 2006

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This paper reviews the concepts, recent history, and current challenges for realizing ultracompact particle accelerators based on surfing on plasma waves. Ideas that seemed fanciful when first proposed by John Dawson in the late 1970s have now come to fruition as a result of the development of ultrashort high-power laser and particle beam drivers, tunnel-ionized plasma sources, and one-to-one particle simulation capability. Breakthroughs in the past 2 years have dramatically advanced the field. Laser-driven gas jets now produce 100 MeV beams of electrons that are monoenergetic and that have transverse beam quality and brightness exceeding that in conventional accelerators. Electron-beam driven plasma waves driven by the 28 GeV electron beam of the Stanford Linear Accelerator Center have been used to accelerate electrons in the tail of the beam by more than 10 GeV in less than 30 cm. The prospects for extending both of these schemes to the energy frontier (currently 50 GeV) and beyond are discussed.
Show PACS
29.20.-c Accelerators
52.38.Ph X-ray, γ-ray, and particle generation
52.40.Mj Particle beam interactions in plasmas
52.75.-d Plasma devices
29.27.Bd Beam dynamics; collective effects and instabilities
29.27.Fh Beam characteristics
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