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An impurity hole observed in the Large Helical Device (LHD) is a hollow density profile of an impurity ion species formed in the core plasma where the negative (inward-pointing) ambipolar radial electric field ($E_r$) exists. Although local…

Impurities cause radiation losses and plasma dilution, and in stellarator plasmas the neoclassical ambipolar radial electric field is often unfavorable for avoiding strong impurity peaking. In this work we use a new continuum drift-kinetic…

Plasma Physics · Physics 2015-11-23 Albert Mollén , Matt Landreman , Håkan M. Smith , Stefanie Braun , Per Helander

The particle transport of impurities in magnetically confined plasmas under some conditions does not find, neither quantitatively nor qualitatively, a satisfactory theory-based explanation. This compromise the successful realization of…

The component of the neoclassical electrostatic potential that is non-constant on the magnetic surface, that we denote by $\tilde\varphi$, can affect radial transport of highly charged impurities, and this has motivated its inclusion in…

Plasma Physics · Physics 2018-09-12 Ivan Calvo , J. L. Velasco , Felix I. Parra , J. Arturo Alonso , J. M. García-Regaña

Achieving impurity and helium ash control is a crucial issue in the path towards fusion-grade magnetic confinement devices, and this is particularly the case of helical reactors, whose low-collisionality ion-root operation scenarios usually…

The control of impurity accumulation is one of the main challenges for future stellarator fusion reactors. The standard argument to explain this accumulation relies on the, in principle, large inward pinch in the neoclassical impurity flux…

Plasma Physics · Physics 2018-11-14 Ivan Calvo , Felix I. Parra , J. L. Velasco , J. Arturo Alonso , J. M. García-Regaña

An enhancement of core impurity transport is observed in high-density plasmas of the stellarator LHD heated by neutral beam injection when continuous lithium (Li) granule dropping is performed. In the experiments reported here, in which the…

In toroidal magnetic confinement devices, such as tokamaks and stellarators, neoclassical transport is usually an order of magnitude larger than its classical counterpart. However, when a high-collisionality species is present in a…

Plasma Physics · Physics 2019-07-31 S. Buller , A. Mollén , S. L. Newton , H. M. Smith , I. Pusztai

Recent developments in theory-based modelling of core heavy impurity transport are presented, and shown to be necessary for quantitative description of present experiments in JET and ASDEX Upgrade. The treatment of heavy impurities is…

High-Z impurities in magnetic confinement devices are prone to develop density variations on the flux-surface, which can significantly affect their transport. In this paper, we generalize earlier analytic stellarator calculations of the…

Plasma Physics · Physics 2019-06-11 S. Buller , H. M. Smith , P. Helander , A. Mollén , S. L. Newton , I. Pusztai

Avoiding impurity accumulation is a requirement for steady-state stellarator operation. The accumulation of impurities can be heavily affected by variations in their density on the flux-surface. Using recently derived semi-analytic…

Plasma Physics · Physics 2019-04-15 Stefan Buller , Håkan M. Smith , Albert Mollén , Sarah Louise Newton , Istvan Pusztai

A potential threat to the performance of magnetically confined fusion plasmas is the problem of impurity accumulation, which causes the concentration of highly charged impurity ions to rise uncontrollably in the center of the plasma and…

Plasma Physics · Physics 2017-04-19 Per Helander , Sarah L. Newton , Albert Mollén , Håkan M. Smith

Main ions influence impurity dynamics through a variety of mechanisms; in particular, via impurity-ion collisions. To lowest order in an expansion in the main ion mass over the impurity mass, the impurity-ion collision operator only depends…

Plasma Physics · Physics 2020-01-08 Ivan Calvo , Felix I. Parra , J. L. Velasco , J. M. García-Regaña

In reactor-relevant plasmas, neoclassical transport drives an outward particle flux in the core of large stellarators and predicts strongly hollow density profiles. However, this theoretical prediction is contradicted by experiments. In…

Impurity temperature screening is a favorable neoclassical phenomenon involving an outward radial flux of impurity ions from the core of fusion devices. Quasisymmetric magnetic fields are intrinsically ambipolar and give rise to temperature…

Plasma Physics · Physics 2020-06-24 Mike F Martin , Matt Landreman

Low-collisionality stellarator plasmas usually display a large negative radial electric field that has been expected to cause accumulation of impurities due to their high charge number. In this paper, two combined effects that can…

We directly optimize stellarator neoclassical ion transport while holding neoclassical electron transport at a moderate level, creating a scenario favorable for impurity expulsion and retaining good ion confinement. Traditional neoclassical…

Plasma Physics · Physics 2024-09-04 B. F. Lee , S. A. Lazerson , H. M. Smith , C. D. Beidler , N. A. Pablant

We present a numerical study of collisional transport in a tokamak pedestal in the presence of non-trace impurities, using the radially global $\delta f$ neoclassical solver PERFECT [M. Landreman et al. 2014 Plasma Phys. Control. Fusion 56…

Plasma Physics · Physics 2016-08-03 I. Pusztai , S. Buller , M. Landreman

The accumulation of impurities in the core of magnetically confined plasmas, resulting from standard collisional transport mechanisms, is a known threat to their performance as fusion energy sources. Whilst the axisymmetric tokamak systems…

Plasma Physics · Physics 2017-11-15 Sarah L. Newton , Per Helander , Albert Mollén , Håkan M. Smith

In tokamak transport barriers, the radial scale of profile variations can be comparable to a typical ion orbit width, which makes the coupling of the distribution function across flux surfaces important in the collisional dynamics. We use…

Plasma Physics · Physics 2017-04-26 Stefan Buller , Istvan Pusztai , Sarah Newton , John Omotani
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