Publications

2015

Towards an emerging understanding of non-locality phenomena and non-local transport
- Ida K.
- Shi Z.
- Sun H. J.
- Inagaki S.
- Kamiya K.
- Rice J.E.
- Tamura N.
- Diamond P.H.
- Dif-Pradalier Guilhem
- Zou X. L.
- Itoh K.
- Sugita S.
- Gürcan Özgür D.
- Estrada T.
- Hidalgo C.
- Hahm T.S.
- Field A.
- Ding X. T.
- Sakamoto Y.
- Oldenburger S.
- Yoshinuma M.
- Kobayashi T.
- Jiang M.
- Hahn S. -H.
- Jeon Y. M.
- Hong S. H.
- Kosuga Y.
- Dong J.
- Itoh S. I.
Nuclear Fusion, IOP Publishing, 2015, 55 (1), pp.013022. In this paper, recent progress on experimental analysis and theoretical models for non-local transport (non-Fickian fluxes in real space) is reviewed. The non-locality in the heat and momentum transport observed in the plasma, the departures from linear flux-gradient proportionality, and externally triggered non-local transport phenomena are described in both L-mode and improved-mode plasmas. Ongoing evaluation of 'fast front' and 'intrinsically non-local' models, and their success in comparisons with experimental data, are discussed (10.1088/0029-5515/55/1/013022)
DOI : 10.1088/0029-5515/55/1/013022
Experimental turbulence studies for gyro-kinetic code validation using advanced microwave diagnostics
- Stroth U.
- Bañón Navarro A.
- Conway G. D.
- Görler T.
- Happel T.
- Hennequin Pascale
- Lechte C.
- Manz P.
- Simon P.
- Biancalani A.
- Blanco E.
- Bottereau C.
- Clairet F.
- Coda S.
- Eibert T.
- Estrada T.
- Fasoli A.
- Guimarais L.
- Gürcan Özgür D.
- Huang Z.
- Jenko F.
- Kasparek W.
- Koenen C.
- Krämer-Flecken A.
- Manso M.-E.
- Medvedeva A.
- Molina D.
- Nikolaeva V.
- Plaum B.
- Porte L.
- Prisiazhniuk D.
- Ribeiro T.
- Scott B.D.
- Siart U.
- Storelli A.
- Vermare Laure
- Wolf S.
Nuclear Fusion, IOP Publishing, 2015, 55 (8), pp.083027. For a comprehensive comparison with theoretical models and advanced numerical turbulence simulations, a large spectrum of fluctuation parameters was measured on the devices ASDEX Upgrade, TCV, and Tore-Supra. Radial profiles of scale-resolved turbulence levels in H-mode discharges are measured and compared with GENE simulations in the transition range from ion-temperature-gradient to trapped-electron-mode turbulence. Correlation reflectometry is used to study the microscopic structure of turbulence and GAMs in discharges where poloidal flow damping was varied by means of variations of the shape of the poloidal plasma cross-section and collisionality. Full-wave codes and synthetic diagnostics are applied for the interpretation of the data. (10.1088/0029-5515/55/8/083027)
DOI : 10.1088/0029-5515/55/8/083027
Some statistical equilibrium mechanics and stability properties of a class of two-dimensional Hamiltonian mean-field models
- Maciel J. M.
- Firpo Marie-Christine
- Amato M. A.
Physica A: Statistical Mechanics and its Applications, Elsevier, 2015, 424, pp.34-43. Abstract A two-dimensional class of mean-field models that may serve as a minimal model to study the properties of long-range systems in two space dimensions is considered. The statistical equilibrium mechanics is derived in the microcanonical ensemble using Monte Carlo simulations for different combinations of the coupling constants in the potential leading to fully repulsive, fully attractive and mixed attractive?repulsive potential along the Cartesian axis and diagonals. Then, having in mind potential realizations of long-range systems using cold atoms, the linear theory of this two-dimensional mean-field Hamiltonian models is derived in the low temperature limit. (10.1016/j.physa.2014.12.030)
DOI : 10.1016/j.physa.2014.12.030
Comprehensive comparisons of geodesic acoustic mode characteristics and dynamics between Tore Supra experiments and gyrokinetic simulations
- Storelli A.
- Vermare Laure
- Hennequin Pascale
- Gürcan Özgür D.
- Dif-Pradalier Guilhem
- Sarazin Y.
- Garbet X.
- Görler T.
- Singh Rameswar
- Morel Pierre
- Grandgirard Virginie
- Ghendrih Philippe
- Tore Supra Team
Physics of Plasmas, American Institute of Physics, 2015, 22 (6). In a dedicated collisionality scan in Tore Supra, the geodesic acoustic mode (GAM) is detected and identified with the Doppler backscattering technique. Observations are compared to the results of a simulation with the gyrokinetic code GYSELA. We found that the GAM frequency in experiments is lower than predicted by simulation and theory. Moreover, the disagreement is higher in the low collisionality scenario. Bursts of non harmonic GAM oscillations have been characterized with filtering techniques, such as the Hilbert-Huang transform. When comparing this dynamical behaviour between experiments and simulation, the probability density function of GAM amplitude and the burst autocorrelation time are found to be remarkably similar. In the simulation, where the radial profile of GAM frequency is continuous, we observed a phenomenon of radial phase mixing of the GAM oscillations, which could influence the burst autocorrelation time. (10.1063/1.4922845)
DOI : 10.1063/1.4922845
Imprints of Expansion on the Local Anisotropy of Solar Wind Turbulence
- Verdini Andrea
- Grappin Roland
The Astrophysical Journal Letters, Bristol : IOP Publishing, 2015, 808, pp.L34. We study the anisotropy of II-order structure functions (SFs) defined in a frame attached to the local mean field in three-dimensional (3D) direct numerical simulations of magnetohydrodynamic turbulence, with the solar wind expansion both included and not included. We simulate spacecraft flybys through the numerical domain by taking increments along the radial (wind) direction that form an angle of 45° with the ambient magnetic field. We find that only when expansion is taken into account do the synthetic observations match the 3D anisotropy observed in the solar wind, including the change of anisotropy with scale. Our simulations also show that the anisotropy changes dramatically when considering increments oblique to the radial directions. Both results can be understood by noting that expansion reduces the radial component of the magnetic field at all scales, thus confining fluctuations in the plane perpendicular to the radial. Expansion is thus shown to affect not only the (global) spectral anisotropy, but also the local anisotropy of second-order SF by influencing the distribution of the local mean field, which enters this higher-order statistics. (10.1088/2041-8205/808/2/L34)
DOI : 10.1088/2041-8205/808/2/L34
Finding the Elusive E × B Staircase in Magnetized Plasmas
- Dif-Pradalier Guilhem
- Hornung G
- Ghendrih Philippe
- Sarazin Yanick
- Clairet F
- Vermare L
- Diamond P H
- Abiteboul J
- Cartier-Michaud T
- Ehrlacher C
- Estève Daniel
- Garbet Xavier
- Grandgirard Virginie
- Gürcan Özgür D.
- Hennequin P
- Kosuga Y
- Latu Guillaume
- Maget P
- Morel Pierre
- Norscini C
- Sabot R
- Storelli A.
Physical Review Letters, American Physical Society, 2015, 114, pp.085004. Turbulence in hot magnetized plasmas is shown to generate permeable localized transport barriers that globally organize into the so-called "ExB staircase" [G. Dif-Pradalier et al., Phys. Rev. E, 82, 025401(R) (2010)]. Its domain of existence and dependence with key plasma parameters is discussed theoretically. Based on these predictions, staircases are observed experimentally in the Tore Supra tokamak by means of high-resolution fast-sweeping X-mode reflectometry. This observation strongly emphasizes the critical role of mesoscale self-organization in plasma turbulence and may have far-reaching consequences for turbulent transport models and their validation. (10.1103/PhysRevLett.114.085004)
DOI : 10.1103/PhysRevLett.114.085004
Is collisionless heating in capacitively coupled plasmas really collisionless?
- Lafleur Trevor
- Chabert Pascal
Plasma Sources Science and Technology, IOP Publishing, 2015, 24 (4), pp.044002. By performing a combination of test-particle and particle-in-cell simulations, we investigate electron heating in single frequency capacitively coupled plasmas (CCPs). In agreement with previous theoretical considerations highlighted in Kaganovich et al (1996 Appl. Phys. Lett. 69 3818), we show that the level of true collisionless/stochastic heating in typical CCPs is significantly smaller than that due to collisional interactions; even at very low pressures and wide gap lengths. Fundamentally electron heating is a collisional phenomenon whereby particle collisions provide the vital phase randomization and stochastization mechanism needed to generate both a local (or ohmic) heating component, and a non-local (or hybrid) heating component. (10.1088/0963-0252/24/4/044002)
DOI : 10.1088/0963-0252/24/4/044002
Structure of a laser-driven radiative shock
- Chaulagain Uddhab
- Stehle Chantal
- Larour Jean
- Kozlová Michaela
- Suzuki-Vidal Francisco
- Barroso Patrice
- Cotelo M.
- Velarde P.
- Rodriguez R.
- Gil J. M.
- Ciardi Andrea
- Acef Ouali
- Nejdl Jaroslav
- de Sá Lionel
- Singh Raj Laxmi
- Ibgui Laurent
- Champion Norbert
High Energy Density Physics, Elsevier, 2015, 17, pp.106-113. Radiative shocks are ubiquitous in stellar environments and are characterized by high temperature plasma emitting a considerable fraction of their energy as radiation. The physical structure of these shocks is complex and experimental benchmarks are needed to provide a deeper understanding of the physics at play. In addition, experiments provide unique data for testing radiation hydrodynamics codes which, in turn, are used to model astrophysical phenomena.
Production of nongyrotropic and gyrotropic backstreaming ion distributions in the quasi-perpendicular ion foreshock region
- Savoini Philippe
- Lembège Bertrand
Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120 (9), pp.7154–7171. A curved shock is analyzed in the whole quasi-perpendicular propagation region (90° ≥ θBn≥45°) in a supercritical regime with the help of a 2-D particle-in-cell code including self-consistent effects such as the shock front curvature and the time-of-flight effects. Two distinct ion populations are observed within the foreshock: a (gyrotropic) field-aligned beam population, hereafter named “FAB,” and a (nongyrotropic) gyrophase bunched population, hereafter named “GPB.” The origin of these high-energy particles and their corresponding acceleration mechanisms are analyzed in details in the present paper. Both FAB and GPB populations are shown to be produced by the shock front itself and more important, do have exactly the same origin. At the shock front, the two populations gain a nongyrotropic distribution, but FAB population loses its initial phase coherency after suffering several bounces along the curved front. This result has one main consequence: the time evolution of the two populations does not involve some distinct reflection processes as often claimed in the literature, but results only from the particle time history at the shock front. This important result was not expected and greatly simplifies the question of their origin. More precisely, a new parameter, the injection angle θinj has been defined between the shock normal direction and the ion gyrating velocity vector. We found that the FAB population is formed by ions injected almost along the shock front, while GPB population is formed by ions injected almost along the shock normal. (10.1002/2015JA021018)
DOI : 10.1002/2015JA021018
Systematic analysis of occurrence of equatorial noise emissions using 10 years of data from the Cluster mission
- Hrbackova Z.
- Santolík O.
- Nemec F.
- Macusova E.
- Cornilleau-Wehrlin Nicole
Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120, pp.1007-1021. We report results of a systematic analysis of equatorial noise (EN) emissions which are also known as fast magnetosonic waves. EN occurs in the vicinity of the geomagnetic equator at frequencies between the local proton cyclotron frequency and the lower hybrid frequency. Our analysis is based on the data collected by the Spatio-Temporal Analysis of Field Fluctuations-Spectrum Analyzer instruments on board the four Cluster spacecraft. The data set covers the period from January 2001 to December 2010. We have developed selection criteria for the visual identification of these emissions, and we have compiled a list of more than 2000 events identified during the analyzed time period. The evolution of the Cluster orbit enables us to investigate a large range of McIlwain's parameter from about L1.1 to L10. We demonstrate that EN can occur at almost all analyzed L shells. However, the occurrence rate is very low (<6%) at L shells below L=2.5 and above L=8.5. EN mostly occurs between L=3 and L=5.5, and within 7° of the geomagnetic equator, reaching 40% occurrence rate. This rate further increases to more than 60% under geomagnetically disturbed conditions. Analysis of occurrence rates as a function of magnetic local time (MLT) shows strong variations outside of the plasmasphere (with a peak around 15 MLT), while the occurrence rate inside the plasmasphere is almost independent on MLT. This is consistent with the hypothesis that EN is generated in the afternoon sector of the plasmapause region and propagates both inward and outward. (10.1002/2014JA020268)
DOI : 10.1002/2014JA020268
WEST Physics Basis
- Bourdelle C.
- Artaud J.F.
- Basiuk Vincent
- Bécoulet M.
- Brémond S.
- Bucalossi J.
- Bufferand H.
- Ciraolo G.
- Colas L.
- Corre Y.
- Courtois X.
- Decker J.
- Delpech L.
- Devynck P.
- Dif-Pradalier Guilhem
- Doerner R.P.
- Douai D.
- Dumont Rémi
- Ekedahl A.
- Fedorczak N.
- Fenzi C.
- Firdaouss M.
- Garcia J.
- Ghendrih Philippe
- Gil C.
- Giruzzi G.
- Goniche M.
- Grisolia C.
- Grosman A.
- Guilhem D.
- Guirlet R.
- Gunn J.
- Hennequin Pascale
- Hillairet J.
- Hoang T.
- Imbeaux Frédéric
- Ivanova-Stanik Irena
- Joffrin E.
- Kallenbach A.
- Linke J.
- Loarer T.
- Lotte P.
- Maget P.
- Marandet Yannick
- Mayoral M.L.
- Meyer O.
- Missirlian M.
- Mollard P.
- Monier-Garbet P.
- Moreau P.
- Nardon Eric
- Pégourié B.
- Peysson Y.
- Sabot R.
- Saint-Laurent F.
- Schneider M.
- Travère J. M.
- Tsitrone E.
- Vartanian S.
- Vermare Laure
- Yoshida M.
- Zagorski R.
- Jet Contributors
Nuclear Fusion, IOP Publishing, 2015, 55 (6), pp.063017. With WEST (Tungsten Environment in Steady State Tokamak) (Bucalossi et al 2014 Fusion Eng. Des. 89 [http://dx.doi.org/10.1016/j.fusengdes.2014.01.062] 907?12 ), the Tore Supra facility and team expertise (Dumont et al 2014 Plasma Phys. Control. Fusion 56 [http://dx.doi.org/10.1088/0741-3335/56/7/075020] 075020 ) is used to pave the way towards ITER divertor procurement and operation. It consists in implementing a divertor configuration and installing ITER-like actively cooled tungsten monoblocks in the Tore Supra tokamak, taking full benefit of its unique long-pulse capability. WEST is a user facility platform, open to all ITER partners. This paper describes the physics basis of WEST: the estimated heat flux on the divertor target, the planned heating schemes, the expected behaviour of the L?H threshold and of the pedestal and the potential W sources. A series of operating scenarios has been modelled, showing that ITER-relevant heat fluxes on the divertor can be achieved in WEST long pulse H-mode plasmas. (10.1088/0029-5515/55/6/063017)
DOI : 10.1088/0029-5515/55/6/063017
Solar illumination control of ionospheric outflow above polar cap arcs
- Maes Lukas
- Maggiolo R.
- de Keyser J.
- Dandouras I.
- Fear R. C.
- Fontaine Dominique
- Haaland S.
Geophysical Research Letters, American Geophysical Union, 2015, 42 (5), pp.1304-1311. We measure the flux density, composition, and energy of outflowing ions above the polar cap, accelerated by quasi-static electric fields parallel to the magnetic field and associated with polar cap arcs, using Cluster. Mapping the spacecraft position to its ionospheric foot point, we analyze the dependence of these parameters on the solar zenith angle (SZA). We find a clear transition at SZA between 94° and 107°, with the O flux higher above the sunlit ionosphere. This dependence on the illumination of the local ionosphere indicates that significant O upflow occurs locally above the polar ionosphere. The same is found for H , but to a lesser extent. This effect can result in a seasonal variation of the total ion upflow from the polar ionosphere. Furthermore, we show that low-magnitude field-aligned potential drops are preferentially observed above the sunlit ionosphere, suggesting a feedback effect of ionospheric conductivity. (10.1002/2014GL062972)
DOI : 10.1002/2014GL062972
Geodesic acoustic modes in a fluid model of tokamak plasma: the effects of finite beta and collisionality
- Singh Rameswar
- Storelli A.
- Gürcan Özgür D.
- Hennequin Pascale
- Vermare Laure
- Morel Pierre
- Singh R.
Plasma Physics and Controlled Fusion, IOP Publishing, 2015, 57, pp.125002. Starting from the Braginskii equations, relevant for the tokamak edge region, a complete set of nonlinear equations for the geodesic acoustic modes (GAM) has been derived which includes collisionality, plasma beta and external sources of particle, momentum and heat. Local linear analysis shows that the GAM frequency increases with collisionality at low radial wave number and decreases at high . GAM frequency also decreases with plasma beta. Radial profiles of GAM frequency for two Tore Supra shots, which were part of a collisionality scan, are compared with these calculations. A discrepancy between experiment and theory is observed, which seems to be explained by a finite for the GAM when flux surface averaged density \langle n\rangle and temperature are assumed to vanish. It is shown that this agreement is incidental and self-consistent inclusion of and responses enhances the disagreement more with at high . So the discrepancy between the linear GAM calculation and experiment, (which also persist for more 'complete' linear models such as gyrokinetics) can probably not be resolved by simply adding a finite . (10.1088/0741-3335/57/12/125002)
DOI : 10.1088/0741-3335/57/12/125002
Plasma acceleration using a radio frequency self-bias effect
- Rafalskyi D.V.
- Aanesland Ane
Physics of Plasmas, American Institute of Physics, 2015, 22 (6), pp.063502. In this work plasma acceleration using a RF self-bias effect is experimentally studied. The experiments are conducted using a novel plasma accelerator system, called Neptune, consisting of an inductively coupled plasma source and a RF-biased set of grids. The plasma accelerator can operate in a steady state mode, producing a plasma flow with separately controlled plasma flux and velocity without any magnetic configuration. The operating pressure at the source output is as low as 0.2 mTorr and can further be decreased. The ion and electron flows are investigated by measuring the ion and electron energy distribution functions both space resolved and with different orientations with respect to the flow direction. It is found that the flow of electrons from the source is highly anisotropic and directed along the ion flow and this global flow of accelerated plasma is well localized in the plasma transport chamber. The maximum flux is about 7.5·1015 ions s−1 m−2 (at standard conditions) on the axis and decreasing to almost zero at a radial distances of more than 15 cm from the flow axis. Varying the RF acceleration voltage in the range 20350 V, the plasma flow velocity can be changed between 10 and 35 km/s. The system is prospective for different technology such as space propulsion and surface modification and also interesting for fundamental studies for space-related plasma simulations and investigation of the dynamo effect using accelerated rotating plasmas. I. INTRODUCT (10.1063/1.4922065)
DOI : 10.1063/1.4922065
Numerical experiment to estimate the validity of negative ion diagnostic using photo-detachment combined with Langmuir probing
- Oudini N.
- Sirse Nishant
- Benallal R.
- Taccogna F.
- Aanesland Ane
- Bendib A.
- Ellingboe A. R.
Physics of Plasmas, American Institute of Physics, 2015, 22 (7), pp.073509. This paper presents a critical assessment of the theory of photo-detachment diagnostic method used to probe the negative ion density and electronegativity α = n-/ne. In this method, a laser pulse is used to photo-detach all negative ions located within the electropositive channel (laser spot region). The negative ion density is estimated based on the assumption that the increase of the current collected by an electrostatic probe biased positively to the plasma is a result of only the creation of photo-detached electrons. In parallel, the background electron density and temperature are considered as constants during this diagnostics. While the numerical experiments performed here show that the background electron density and temperature increase due to the formation of an electrostatic potential barrier around the electropositive channel. The time scale of potential barrier rise is about 2 ns, which is comparable to the time required to completely photo-detach the negative ions in the electropositive channel (∼3 ns). We find that neglecting the effect of the potential barrier on the background plasma leads to an erroneous determination of the negative ion density. Moreover, the background electron velocity distribution function within the electropositive channel is not Maxwellian. This is due to the acceleration of these electrons through the electrostatic potential barrier. In this work, the validity of the photo-detachment diagnostic assumptions is questioned and our results illustrate the weakness of these assumptions. (10.1063/1.4926826)
DOI : 10.1063/1.4926826
Reply to Comment on "A review on ion-ion plasmas created in weakly magnetized electronegative plasmas
- Aanesland Ane
- Bredin Jérôme
- Chabert Pascal
Plasma Sources Science and Technology, IOP Publishing, 2015, 24 (3), pp.038002. This is a reply to the comments made by Bogdanov et al on our paper entitled ?A review on ion?ion plasmas created in weakly magnetized electronegative plasmas?. We have clarified some issues regarding the electronegative plasma stratification and the definition of an ion?ion plasma, and we discuss the issue of extracting negative ions from a steady-state ion?ion plasma formed at the periphery or downstream a magnetized electronegative plasma. (10.1088/0963-0252/24/3/038002)
DOI : 10.1088/0963-0252/24/3/038002
Magnetic reconnection in th Solar System
- Aunai N.
, 2015.
Kinetic simulations of secondary reconnection in the reconnection jet
- Huang S. Y.
- Zhou M.
- Yuan Z. G.
- Fu H.S.
- He J. S.
- Sahraoui Fouad
- Aunai Nicolas
- Deng X. H.
- Fu S. Y.
- Pang Y.
- Wang D. D.
Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120 (8), pp.61886198. Magnetic reconnection, as one important energy dissipation process in plasmas, has been extensively studied in the past several decades. Magnetic reconnection occurring in the downstream of a primary X line is referred to as secondary reconnection. In this paper, we used kinetic simulations to investigate the secondary reconnection in detail. We found that secondary reconnection is reversed by the compression caused by the outflowing jet originating from the primary reconnection site, which results in the erosion of the magnetic island between the two X lines within ~3 ωci−1. We show the observational signatures expected in electromagnetic fields and plasma measurements in the Earth's magnetotail, associated with this mechanism. These simulation results could be applied to interpret the signatures associated with the evolution of earthward magnetic islands in the Earth's magnetotail. (10.1002/2014JA020969)
DOI : 10.1002/2014JA020969
What is the nature of magnetosheath FTEs?
- Roux A.
- Robert Patrick
- Fontaine Dominique
- Le Contel Olivier
- Canu Patrick
- Louarn P.
Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120 (6), pp.4576-4595. Cluster multipoint measurements are used to study two successive magnetosheath flux transfer events (FTEs). Magnetic field lines in the leading region are found to be closed magnetospheric field lines. For event 1 these field lines are wounded up by a large current structure oriented eastward and moving poleward. Conversely, the trailing region corresponds to opened magnetic field lines. For both events the leading edge of the FTEs is a tangential discontinuity separating the magnetosheath from closed field lines. In the case of event 1 magnetosheath ions are accelerated through the FTE trailing edge via a rotational discontinuity and penetrate on closed field lines through a second discontinuity. Thus, the ion jet is accelerated equatorward of the spacecraft but the backtracking of the discontinuities and the lack of dispersion show that ion acceleration occurs at less than 2 RE from Cluster. On the other hand the extrapolation forward indicates that the FTE bulge steepens as in simulations of Dorelli and Bhattacharjee). Evidence is given for the penetration of magnetosheath ions inside the core of the FTE, on closed field lines. Magnetosheath electrons are accelerated in parallel and antiparallel directions on open and on closed field lines, thus breaking the frozen-in condition. Event 2 is also split in two distinct regions but no evidence is found for accelerated bidirectional magnetosheath electrons. For event 2 the two discontinuities at the trailing region are stacked together when they are crossed by the spacecraft, suggesting that the current splitting is a reconnection signature. (10.1002/2015JA020983)
DOI : 10.1002/2015JA020983
Kinetic scale turbulence and dissipation in the solar wind: key observational results and future outlook
- Goldstein M. L.
- Wicks R. T.
- Perri S.
- Sahraoui Fouad
Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences, Royal Society, The, 2015, 373, pp.20140147. Turbulence is ubiquitous in the solar wind. Turbulence causes kinetic and magnetic energy to cascade to small scales where they are eventually dissipated, adding heat to the plasma. The details of how this occurs are not well understood. This article reviews the evidence for turbulent dissipation and examines various diagnostics for identifying solar wind regions where dissipation is occurring. We also discuss how future missions will further enhance our understanding of the importance of turbulence to solar wind dynamics. (10.1098/rsta.2014.0147)
DOI : 10.1098/rsta.2014.0147
Gyrokinetic turbulence cascade via predator-prey interactions between different scales
- Kobayashi Sumire
- Gürcan Özgür D.
Physics of Plasmas, American Institute of Physics, 2015, 22 (5), pp.050702. Gyrokinetic simulations in a closed fieldline geometry are presented to explore the physics of nonlinear transfer in plasma turbulence. As spontaneously formed zonal flows and small-scale turbulence demonstrate predator-prey dynamics, a particular cascade spectrum emerges. The electrostatic potential and the density spectra appear to be in good agreement with the simple theoretical prediction based on Charney-Hasegawa-Mima equation |||ϕ̃k|||2∼||ñk||2∝k−3/(1 k2)2, with the spectra becoming anisotropic at small scales. The results indicate that the disparate scale interactions, in particular, the refraction and shearing of larger scale eddies by the self-consistent zonal flows, dominate over local interactions, and contrary to the common wisdom, the comprehensive scaling relation is created even within the energy injection region. (10.1063/1.4920965)
DOI : 10.1063/1.4920965
Polarization analysis of CuXX-lines emitted from X-pinch
- Baronova E O
- Larour Jean
- Rosmej F B
- Khattak F y
Journal of Physics: Conference Series, IOP Science, 2015, 653, pp.012145. Soft x-ray emission from CuXX L-shell lines emitted by a dense X-pinch plasma have been investigated with high-resolution curved Bragg crystals at different angles of orientation. Single shot time integrated spectra show clear evidences of polarization for the Ne-like spectral lines 2s22p6 1S0 → 2s22p53s 1P1 (λ = 12.570 Å), 2s22p6 1S0 → 2s22p53s 3P1 (λ = 12.8277 Å). The variation of the intensity ratio of these two well-separated L-shell lines is discussed in view of its application for suprathermal electron characterization under real experimental conditions of pinch plasmas. We demonstrated that the simultaneous use of two different polarization spectrometers (means 4 Bragg crystals) permitted a high level of confidence for the analysis of the variation of the line ratios due to polarization. (10.1088/1742-6596/653/1/012145)
DOI : 10.1088/1742-6596/653/1/012145
Nature of the MHD and Kinetic Scale Turbulence in the Magnetosheath of Saturn: Cassini Observations
- Hadid Lina
- Sahraoui Fouad
- Kiyani K. H.
- Retinò Alessandro
- Modolo Ronan
- Canu Patrick
- Masters Adam
- Dougherty Michele K.
The Astrophysical Journal Letters, Bristol : IOP Publishing, 2015, 813 (2), pp.L29. Low-frequency turbulence in Saturn's magnetosheath is investigated using in situ measurements of the Cassini spacecraft. Focus is put on the magnetic energy spectra. A set of 42 time intervals in the magnetosheath were analyzed, and three main results that contrast with known features of solar wind turbulence are reported. (10.1088/2041-8205/813/2/L29)
DOI : 10.1088/2041-8205/813/2/L29
Further details on the plasma E × B staircase
- Dif-Pradalier Guilhem
- Hornung G
- Ghendrih Philippe
- Sarazin Yanick
- Clairet F
- Vermare L
- Diamond P H
- Abiteboul J
- Cartier-Michaud T
- Ehrlacher C
- Esteve D
- Garbet Xavier
- Grandgirard Virginie
- Gürcan Özgür D.
- Hennequin P
- Kosuga A
- Latu Guillaume
- Morel Pierre
- Norscini C
- Sabot R
- Storelli A.
, 2015. Turbulence in hot magnetised plasmas spontaneously has been shown to spontaneously organise on global scales into the so-called " E × B staircase ". Further characterisation of this structure is detailed below.
Matched dipole probe for magnetized low electron density laboratory plasma diagnostics
- Rafalskyi D.V.
- Aanesland Ane
Physics of Plasmas, American Institute of Physics, 2015, 22 (7), pp.073504. In this paper, a diagnostic method for magnetized and unmagnetized laboratory plasma is proposed, based on impedance measurements of a short matched dipole. The range of the measured electron densities is limited to low density plasmas (10121015 m−3), where other diagnostic methods have strong limitations on the magnetic field strength and topology, plasma dimensions, and boundary conditions. The method is designed for use in both large- and small-dimension plasma (<10 cm) without or with strong non-homogeneous magnetic field, which can be undefined within the probe size. The design of a matched dipole probe allows to suppress the sheath resonance effects and to reach high sensitivity at relatively small probe dimensions. Validation experiments are conducted in both magnetized (B ∼ 170 G) and unmagnetized (B = 0) low density (7 × 1012 m−37 × 1013 m−3) low pressure (1 mTorr) 10 cm scale plasmas. The experimentally measured data show very good agreement with an analytical theory both for a non-magnetized and a magnetized case. The electron density measured by the matched dipole and Langmuir probes in the range of 7 × 1012 m−37 × 1013 m−3 show less than 30% difference. An experimentally measured tolerance/uncertainty of the dipole probe method is estimated to ±1% for plasma densities above 2 × 1013 m−3. A spatial resolution is estimated from the experiments to be about 3d, where d is the dipole diameter. The diagnostic method is also validated by comparing the measured plasma impedance curves with results of analytical modelling. (10.1063/1.4926447)
DOI : 10.1063/1.4926447

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