Share

Publications

2015

  • Turbulence elasticity: a key concept to a unified paradigm of L -> I -> H transition
    • Guo Z. B.
    • Diamond P.H.
    • Kosuga Y.
    • Gürcan Özgür D.
    Nuclear Fusion, IOP Publishing, 2015, 55 (4), pp.043022. We present a theory of turbulence elasticity, which follows from delayed response of drift waves (DWs) to zonal flow (ZF) shears. It is shown that when |&#12296;V&#12297;'ZF|/&#916;&#969;k &#8805; 1, with |&#12296;V&#12297;'ZF| the ZF shearing rate and &#916;&#969;k the local turbulence decorrelation rate, the ZF evolution equation is converted from a diffusion equation to a telegraph equation. This insight provides a natural framework for understanding temporally periodic ZF structures, e.g., propagation of the ZF/turbulence intensity fronts. Furthermore, by incorporating the elastic property of the DWZF turbulence, we propose a unified paradigm of low-confinement-mode to intermediate-confinement-mode to high-confinement-mode (L &#8594; I &#8594; H) transitions. In particular, we predict the onset and termination conditions of the limit cycle oscillations, i.e. the I-mode. The transition from an unstable L-mode to I-mode is predicted to occur when &#916;&#969;k < |&#12296;V&#12297;'ZF|<&#12296;V&#12297;'cr, where &#12296;V&#12297;'cr is a critical flow shearing rate and is derived explicitly. If |&#12296;V&#12297;'E×B| > &#12296;V&#12297;'cr(&#12296;V&#12297;E×B is mean E × B shear flow driven by edge radial electrostatic field), the I-mode will terminate and spiral into the H-mode. (10.1088/0029-5515/55/4/043022)
    DOI : 10.1088/0029-5515/55/4/043022
  • Direct identification of predator-prey dynamics in gyrokinetic simulations
    • Kobayashi Sumire
    • Gürcan Özgür D.
    • Diamond P.H.
    Physics of Plasmas, American Institute of Physics, 2015, 22 (9), pp.090702. The interaction between spontaneously formed zonal flows and small-scale turbulence in nonlinear gyrokinetic simulations is explored in a shearless closed field line geometry. It is found that when clear limit cycle oscillations prevail, the observed turbulent dynamics can be quantitatively captured by a simple Lotka-Volterra type predator-prey model. Fitting the time traces of full gyrokinetic simulations by such a reduced model allows extraction of the model coefficients. Scanning physical plasma parameters, such as collisionality and density gradient, it was observed that the effective growth rates of turbulence (i.e., the prey) remain roughly constant, in spite of the higher and varying level of primary mode linear growth rates. The effective growth rate that was extracted corresponds roughly to the zonal-flow-modified primary mode growth rate. It was also observed that the effective damping of zonal flows (i.e., the predator) in the parameter range, where clear predator-prey dynamics is observed, (i.e., near marginal stability) agrees with the collisional damping expected in these simulations. This implies that the Kelvin-Helmholtz-like instability may be negligible in this range. The results imply that when the tertiary instability plays a role, the dynamics becomes more complex than a simple Lotka-Volterra predator prey. (10.1063/1.4930127)
    DOI : 10.1063/1.4930127
  • Strong Ionization Asymmetry in a Geometrically Symmetric Radio Frequency Capacitively Coupled Plasma Induced by Sawtooth Voltage Waveforms
    • Bruneau Bastien
    • Gans T.
    • O'Connell D.
    • Greb Arthur
    • Johnson E.V.
    • Booth Jean-Paul
    Physical Review Letters, American Physical Society, 2015, 114, pp.125002. The ionization dynamics in geometrically symmetric parallel plate capacitively coupled plasmas driven by radio frequency tailored voltage waveforms is investigated using phase resolved optical emission spectroscopy (PROES) and particle-in-cell (PIC) simulations. Temporally asymmetric waveforms induce spatial asymmetries and offer control of the spatiotemporal dynamics of electron heating and associated ionization structures. Sawtooth waveforms with different rise and fall rates are employed using truncated Fourier series approximations of an ideal sawtooth. Experimental PROES results obtained in argon plasmas are compared with PIC simulations, showing excellent agreement. With waveforms comprising a fast voltage drop followed by a slower rise, the faster sheath expansion in front of the powered electrode causes strongly enhanced ionization in this region. The complementary waveform causes an analogous effect in front of the grounded electrode. (10.1103/PhysRevLett.114.125002)
    DOI : 10.1103/PhysRevLett.114.125002
  • Magnetic noise contribution of the ferromagnetic core of induction magnetometers
    • Coillot C
    • El Moussalim M
    • Brun E
    • Rhouni A
    • Lebourgeois R
    • Sou Gérard
    • Mansour Malik
    Journal of Sensors and Sensor Systems, Copernicus Publ, 2015, 4, pp.229 - 237. The performance of induction magnetometers, in terms of resolution, depends both on the induction sensor and the electronic circuit. To investigate accurately the sensor noise sources, an induction sensor, made of a ferrite ferromagnetic core, is combined with a dedicated low voltage and current noise preamplifier, designed in CMOS 0.35 µm technology. A modelling of the contribution of the ferromagnetic core to the noise through the complex permeability formalism is performed. Its comparison with experimental measurements highlight another possible source for the dominating noise near the resonance. (10.5194/jsss-4-229-2015)
    DOI : 10.5194/jsss-4-229-2015
  • Wide-banded NTC radiation: local to remote observations by the four Cluster satellites
    • Décréau Pierrette
    • Aoutou S.
    • Denazelle A.
    • Galkina I.
    • Rauch Jean-Louis
    • Vallières Xavier
    • Canu Patrick
    • Rochel Grimald S.
    • El-Lemdani Mazouz Farida
    • Darrouzet F.
    Annales Geophysicae, European Geosciences Union, 2015, 33 (10), pp.1285-1300. The Cluster multi-point mission offers a unique collection of non-thermal continuum (NTC) radio waves observed in the 2-80 kHz frequency range over almost 15 years, from various view points over the radiating plasmasphere. Here we present rather infrequent case events, such as when primary electrostatic sources of such waves are embedded within the plasmapause boundary far from the magnetic equatorial plane. The spectral signature of the emitted electromagnetic waves is structured as a series of wide harmonic bands within the range covered by the step in plasma frequency encountered at the boundary. Developing the concept that the frequency distance df between harmonic bands measures the magnetic field magnitude B at the source (df = F<SUB>ce</SUB>, electron gyrofrequency), we analyse three selected events. The first one (studied in Grimald et al., 2008) presents electric field signatures observed by a Cluster constellation of small size (~ 200 to 1000 km spacecraft separation) placed in the vicinity of sources. The electric field frequency spectra display frequency peaks placed at frequencies fs = n df (n being an integer), with df of the order of F<SUB>ce</SUB> values encountered at the plasmapause by the spacecraft. The second event, taken from the Cluster tilt campaign, leads to a 3-D view of NTC waves ray path orientations and to a localization of a global source region at several Earth radii (R<SUB>E</SUB>) from Cluster (Décréau et al., 2013). The measured spectra present successive peaks placed at fs ~ (n 1/2) df. Next, considering if both situations might be two facets of the same phenomenon, we analyze a third event. The Cluster fleet, configured into a constellation of large size (~ 8000 to 25 000 km spacecraft separation), allows us to observe wide-banded NTC waves at different distances from their sources. Two new findings can be derived from our analysis. First, we point out that a large portion of the plasmasphere boundary layer, covering a large range of magnetic latitudes, is radiating radio waves. The radio waves are issued from multiple sources of small size, each related to a given fs series and radiating inside a beam of narrow cone angle, referred to as a beamlet. The beamlets illuminate different satellites simultaneously, at different characteristic fs values, according to the latitude at which the satellite is placed. Second, when an observing satellite moves away from its assumed source region (the plasmapause surface), it is illuminated by several beamlets, issued from nearby sources with characteristic fs values close to each other. The addition of radio waves blurs the spectra of the overall received electric field. It can move the signal peaks such that their position fs satisfiesfs = (n alpha) df, with 0 < alpha < 1. These findings open new perspectives for the interpretation of NTC events displaying harmonic signatures. (10.5194/angeo-33-1285-2015)
    DOI : 10.5194/angeo-33-1285-2015
  • 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
  • Thin Current Sheets and Associated Electron Heating in Turbulent Space Plasma
    • Chasapis A.
    • Retinò Alessandro
    • Sahraoui Fouad
    • Vaivads A.
    • Khotyaintsev Y. V.
    • Sundkvist D.
    • Greco A.
    • Sorriso-Valvo L.
    • Canu Patrick
    The Astrophysical Journal Letters, Bristol : IOP Publishing, 2015, 804 (1). Intermittent structures, such as thin current sheets, are abundant in turbulent plasmas. Numerical simulations indicate that such current sheets are important sites of energy dissipation and particle heating occurring at kinetic scales. However, direct evidence of dissipation and associated heating within current sheets is scarce. Here, we show a new statistical study of local electron heating within proton-scale current sheets by using high-resolution spacecraft data. Current sheets are detected using the Partial Variance of Increments (PVI) method which identifies regions of strong intermittency. We find that strong electron heating occurs in high PVI (>3) current sheets while no significant heating occurs in low PVI cases (<3), indicating that the former are dominant for energy dissipation. Current sheets corresponding to very high PVI (>5) show the strongest heating and most of the time are consistent with ongoing magnetic reconnection. This suggests that reconnection is important for electron heating and dissipation at kinetic scales in turbulent plasmas. (10.1088/2041-8205/804/1/L1)
    DOI : 10.1088/2041-8205/804/1/L1
  • Entanglement of helicity and energy in kinetic Alfvén wave/whistler turbulence
    • Galtier Sébastien
    • Meyrand Romain
    Journal of Plasma Physics, Cambridge University Press (CUP), 2015, 81 (1), pp.325810106. The role of magnetic helicity is investigated in kinetic Alfvén wave and oblique whistler turbulence in presence of a relatively intense external magnetic field b <SUB>0</SUB> e <SUB>||</SUB>. In this situation, turbulence is strongly anisotropic and the fluid equations describing both regimes are the reduced electron magnetohydrodynamics (REMHD) whose derivation, originally made from the gyrokinetic theory, is also obtained here from compressible Hall magnetohydrodynamics (MHD). We use the asymptotic equations derived by Galtier and Bhattacharjee (2003 Phys. Plasmas 10, 3065-3076) to study the REMHD dynamics in the weak turbulence regime. The analysis is focused on the magnetic helicity equation for which we obtain the exact solutions: they correspond to the entanglement relation, n ñ = -6, where n and ñ are the power law indices of the perpendicular (to b <SUB>0</SUB>) wave number magnetic energy and helicity spectra, respectively. Therefore, the spectra derived in the past from the energy equation only, namely n = -2.5 and ñ = -3.5, are not the unique solutions to this problem but rather characterize the direct energy cascade. The solution ñ = -3 is a limit imposed by the locality condition; it is also the constant helicity flux solution obtained heuristically. The results obtained offer a new paradigm to understand solar wind turbulence at sub-ion scales where it is often observed that -3 < n < -2.5. (10.1017/S0022377814000774)
    DOI : 10.1017/S0022377814000774
  • Different types of whistler mode chorus in the equatorial source region
    • Taubenschuss U.
    • Santolík O.
    • Graham Daniel B.
    • Fu H.S.
    • Khotyaintsev Y. V.
    • Le Contel Olivier
    Geophysical Research Letters, American Geophysical Union, 2015, 42 (20), pp.8271-8279. The Time History of Events and Macroscale Interactions during Substorms-D spacecraft crossed an active equatorial source region of whistler mode chorus rising tones on 23 October 2008. Rising tones are analyzed in terms of spectral and polarization characteristics, with special emphasis on wave normal angles. The latter exhibit large variations from quasi-parallel to oblique, even within single bursts, but seem to follow a definite pattern, which enables an unambiguous classification into five different groups. Furthermore, we discuss the frequently observed splitting of chorus bursts into a lower and an upper band around one half of the local electron cyclotron frequency. At chorus frequencies close to the gap, we find significantly lowered wave planarities and a tendency of wave normal angles to approach the Gendrin angle. (10.1002/2015GL066004)
    DOI : 10.1002/2015GL066004
  • 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
  • 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
  • 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
  • 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
  • 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
  • Observations of discrete harmonics emerging from equatorial noise
    • Balikhin M. A.
    • Shprits Y. Y.
    • Walker S. N.
    • Chen Lunjin
    • Cornilleau-Wehrlin Nicole
    • Dandouras Iannis
    • Santolík O.
    • Carr Christopher
    • Yearby K. H.
    • Weiss Benjamin
    Nature Communications, Nature Publishing Group, 2015, 6. A number of modes of oscillations of particles and fields can exist in space plasmas. Since the early 1970s, space missions have observed noise-like plasma waves near the geomagnetic equator known as `equatorial noise'. Several theories were suggested, but clear observational evidence supported by realistic modelling has not been provided. Here we report on observations by the Cluster mission that clearly show the highly structured and periodic pattern of these waves. Very narrow-banded emissions at frequencies corresponding to exact multiples of the proton gyrofrequency (frequency of gyration around the field line) from the 17th up to the 30th harmonic are observed, indicating that these waves are generated by the proton distributions. Simultaneously with these coherent periodic structures in waves, the Cluster spacecraft observes `ring' distributions of protons in velocity space that provide the free energy for the waves. Calculated wave growth based on ion distributions shows a very similar pattern to the observations. (10.1038/ncomms8703)
    DOI : 10.1038/ncomms8703
  • 3D hybrid simulations of the interaction of a magnetic cloud with a bow shock
    • Turc Lucile
    • Fontaine Dominique
    • Savoini Philippe
    • Modolo Ronan
    Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120 (8), pp.6133-6151. In this paper, we investigate the interaction of a magnetic cloud (MC) with a planetary bow shock using hybrid simulations. It is the first time to our knowledge that this interaction is studied using kinetic simulations which include self-consistently both the ion foreshock and the shock wave dynamics. We show that when the shock is in a quasi-perpendicular configuration, the MC's magnetic structure in the magnetosheath remains similar to that in the solar wind, whereas it is strongly altered downstream of a quasi-parallel shock. The latter can result in a reversal of the magnetic field north-south component in some parts of the magnetosheath. We also investigate how the MC affects in turn the outer parts of the planetary environment, i.e., from the foreshock to the magnetopause. We find the following: (i) The decrease of the Alfvén Mach number at the MC's arrival causes an attenuation of the foreshock region because of the weakening of the bow shock. (ii) The foreshock moves along the bow shock's surface, following the rotation of the MC's magnetic field. (iii) Owing to the low plasma beta, asymmetric flows arise inside the magnetosheath, due to the magnetic tension force which accelerates the particles in some parts of the magnetosheath and slows them down in others. (iv) The quasi-parallel region forms a depression in the shock's surface. Other deformations of the magnetopause and the bow shock are also highlighted. All these effects can contribute to significantly modify the solar wind/magnetosphere coupling during MC events. (10.1002/2015JA021318)
    DOI : 10.1002/2015JA021318
  • Equatorial noise emissions with quasiperiodic modulation of wave intensity
    • Nemec F.
    • Santolík O.
    • Hrbackova Z.
    • Pickett J. S.
    • Cornilleau-Wehrlin Nicole
    Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120, pp.2649-2661. Equatorial noise (EN) emissions are electromagnetic wave events at frequencies between the proton cyclotron frequency and the lower hybrid frequency observed in the equatorial region of the inner magnetosphere. They propagate nearly perpendicular to the ambient magnetic field, and they exhibit a harmonic line structure characteristic of the proton cyclotron frequency in the source region. However, they were generally believed to be continuous in time. We investigate more than 2000 EN events observed by the Spatio-Temporal Analysis of Field Fluctuations and Wide-Band Data Plasma Wave investigation instruments on board the Cluster spacecraft, and we show that this is not always the case. A clear quasiperiodic (QP) time modulation of the wave intensity is present in more than 5% of events. We perform a systematic analysis of these EN events with QP modulation of the wave intensity. Such events occur usually in the noon-to-dawn magnetic local time sector. Their occurrence seems to be related to the increased geomagnetic activity, and it is associated with the time intervals of enhanced solar wind flow speeds. The modulation period of these events is on the order of minutes. Compressional ULF magnetic field pulsations with periods about double the modulation periods of EN wave intensity and magnitudes on the order of a few tenths of nanotesla were identified in about 46% of events. We suggest that these compressional magnetic field pulsations might be responsible for the observed QP modulation of EN wave intensity, in analogy to formerly reported VLF whistler mode QP events. (10.1002/2014JA020816)
    DOI : 10.1002/2014JA020816
  • 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&#8201;&#969;ci&#8722;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
  • 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
  • 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 R<SUB>E</SUB> 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
  • 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
  • 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 |||&#981;&#771;k|||2&#8764;||n&#771;k||2&#8733;k&#8722;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
  • 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&#8201;m&#8722;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&#8201;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&#8201;&#8764;&#8201;170&#8201;G) and unmagnetized (B&#8201;=&#8201;0) low density (7&#8201;×&#8201;1012&#8201;m&#8722;37&#8201;×&#8201;1013&#8201;m&#8722;3) low pressure (1 mTorr) 10&#8201;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&#8201;×&#8201;1012&#8201;m&#8722;37&#8201;×&#8201;1013&#8201;m&#8722;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&#8201;×&#8201;1013&#8201;m&#8722;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
  • 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.
  • The Plasma E × B Staircase: Turbulence Self-Regulation through Spontaneous Flow Patterning
    • Dif-Pradalier Guilhem
    • Hornung G
    • Ghendrih Philippe
    • Clairet R
    • Diamond P H
    • Sarazin Yanick
    • Vermare L
    • Abiteboul J
    • Cartier-Michaud T
    • Ehrlacher C
    • Estève D
    • Garbet Xavier
    • Grandgirard Virginie
    • Gürcan Özgür D.
    • Hennequin P
    • Kosuga Y
    • Latu Guillaume
    • Morel Pierre
    • Norscini C
    • Sabot R
    , 2015. The E × B staircase [1, 2] is a spontaneously formed, turbulence-driven self-organising pattern of quasi-regular, long-lived and localised shear flow [3] and stress layers. These layers coincide with long-lived pressure corrugations and are interspersed between regions of turbulent avalanching. The typical spacing between these layers is mesoscale, noted ∆ ∼ 25 − 30ρ i [1, 4] —in-between the turbulence auto-correlation length c ∼ 5ρ i at micro scales and the profile macroscale L 100ρ i , see e.g. Fig.2 in [1]— and sets the outer scale of the turbulent avalanching. Here ρ i is ion Larmor radius. Whilst arresting, statistically, to mesoscales the detrimental avalanching these layers, located at the " steps of the staircase " are beneficial to confinement. The E×B staircase is thus best understood as a self-organising and dynamical set of weak or permeable transport barriers. Strong mean zonal flows are generated and endure at the steps of the staircase, resulting in localised deviations of the poloidal flow from its oft-assumed neoclassical prediction [5].