Laboratoire pour l'utilisation des lasers intenses

Publications

Publications

2022 | 2021 | 2020 | 2019

Below, by year, are the publications listed in the HAL open archive.

2015

  • Magnetic reconnection in th Solar System
    • Aunai N.
    , 2015.
  • 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
  • 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
  • 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
  • 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
  • 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
  • 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
  • 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
  • Distribution of energetic oxygen and hydrogen in the near-Earth plasma sheet
    • Kronberg E. A.
    • Grigorenko E. E.
    • Haaland S. E.
    • Daly P. W.
    • Delcourt Dominique C.
    • Luo H.
    • Kistler L. M.
    • Dandouras I.
    Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120 (5), pp.3415-3431. The spatial distributions of different ion species are useful indicators for plasma sheet dynamics. In this statistical study based on 7 years of Cluster observations, we establish the spatial distributions of oxygen ions and protons at energies from 274 to 955 keV, depending on geomagnetic and solar wind (SW) conditions. Compared with protons, the distribution of energetic oxygen has stronger dawn-dusk asymmetry in response to changes in the geomagnetic activity. When the interplanetary magnetic field (IMF) is directed southward, the oxygen ions show significant acceleration in the tail plasma sheet. Changes in the SW dynamic pressure (P<SUB>dyn</SUB>) affect the oxygen and proton intensities in the same way. The energetic protons show significant intensity increases at the near-Earth duskside during disturbed geomagnetic conditions, enhanced SW P<SUB>dyn</SUB>, and southward IMF, implying there location of effective inductive acceleration mechanisms and a strong duskward drift due to the increase of the magnetic field gradient in the near-Earth tail. Higher losses of energetic ions are observed in the dayside plasma sheet under disturbed geomagnetic conditions and enhanced SW P<SUB>dyn</SUB>. These observations are in agreement with theoretical models. (10.1002/2014JA020882)
    DOI : 10.1002/2014JA020882
  • Asymmetric kinetic equilibria: Generalization of the BAS model for rotating magnetic profile and non-zero electric field
    • Dorville Nicolas
    • Belmont Gérard
    • Aunai Nicolas
    • Dargent Jérémy
    • Rezeau Laurence
    Physics of Plasmas, American Institute of Physics, 2015, 22 (9), pp.092904. Finding kinetic equilibria for non-collisional/collisionless tangential current layers is a key issue as well for their theoretical modeling as for our understanding of the processes that disturb them, such as tearing or Kelvin Helmholtz instabilities. The famous Harris equilibrium [E. Harris, Il Nuovo Cimento Ser. 10 23, 115121 (1962)] assumes drifting Maxwellian distributions for ions and electrons, with constant temperatures and flow velocities; these assumptions lead to symmetric layers surrounded by vacuum. This strongly particular kind of layer is not suited for the general case: asymmetric boundaries between two media with different plasmas and different magnetic fields. The standard method for constructing more general kinetic equilibria consists in using Jeans theorem, which says that any function depending only on the Hamiltonian constants of motion is a solution to the steady Vlasov equation [P. J. Channell, Phys. Fluids (19581988) 19, 1541 (1976); M. Roth et al., Space Sci. Rev. 76, 251317 (1996); and F. Mottez, Phys. Plasmas 10, 15411545 (2003)]. The inverse implication is however not true: when using the motion invariants as variables instead of the velocity components, the general stationary particle distributions keep on depending explicitly of the position, in addition to the implicit dependence introduced by these invariants. The standard approach therefore strongly restricts the class of solutions to the problem and probably does not select the most physically reasonable. The BAS (Belmont-Aunai-Smets) model [G. Belmont et al., Phys. Plasmas 19, 022108 (2012)] used for the first time the concept of particle accessibility to find new solutions: considering the case of a coplanar-antiparallel magnetic field configuration without electric field, asymmetric solutions could be found while the standard method can only lead to symmetric ones. These solutions were validated in a hybrid simulation [N. Aunai et al., Phys. Plasmas (1994-present) 20, 110702 (2013)], and more recently in a fully kinetic simulation as well [J. Dargent and N. Aunai, Phys. Plasmas (submitted)]. Nevertheless, in most asymmetric layers like the terrestrial magnetopause, one would indeed expect a magnetic field rotation from one direction to another without going through zero [J. Berchem and C. T. Russell, J. Geophys. Res. 87, 81398148 (1982)], and a non-zero normal electric field. In this paper, we propose the corresponding generalization: in the model presented, the profiles can be freely imposed for the magnetic field rotation (although restricted to a 180 rotation hitherto) and for the normal electric field. As it was done previously, the equilibrium is tested with a hybrid simulation. (10.1063/1.4930210)
    DOI : 10.1063/1.4930210
  • A Review of General Physical and Chemical Processes Related to Plasma Sources and Losses for Solar System Magnetospheres
    • Seki K.
    • Nagy A.
    • Jackman C. M.
    • Crary F.
    • Fontaine Dominique
    • Zarka P.
    • Wurz Peter
    • Milillo A.
    • Slavin J. A.
    • Delcourt Dominique C.
    • Wiltberger M.
    • Ilie R.
    • Jia X.
    • Ledvina S. A.
    • Liemohn M. W.
    • Schunk R. W.
    Space Science Reviews, Springer Verlag, 2015, 192 (1-4), pp.27-89. The aim of this paper is to provide a review of general processes related to plasma sources, their transport, energization, and losses in the planetary magnetospheres. We provide background information as well as the most up-to-date knowledge of the comparative studies of planetary magnetospheres, with a focus on the plasma supply to each region of the magnetospheres. This review also includes the basic equations and modeling methods commonly used to simulate the plasma sources of the planetary magnetospheres. In this paper, we will describe basic and common processes related to plasma supply to each region of the planetary magnetospheres in our solar system. First, we will describe source processes in Sect. 1. Then the transport and energization processes to supply those source plasmas to various regions of the magnetosphere are described in Sect. 2. Loss processes are also important to understand the plasma population in the magnetosphere and Sect. 3 is dedicated to the explanation of the loss processes. In Sect. 4, we also briefly summarize the basic equations and modeling methods with a focus on plasma supply processes for planetary magnetospheres. (10.1007/s11214-015-0170-y)
    DOI : 10.1007/s11214-015-0170-y
  • 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
  • Predator-prey model for the self-organization of stochastic oscillators in dual populations.
    • Moradi S.
    • Anderson J.
    • Gürcan Özgür D.
    Physical Review E, American Physical Society (APS), 2015, 92, pp.06293. A predator-prey model of dual populations with stochastic oscillators is presented. A linear cross-coupling between the two populations is introduced following the coupling between the motions of a Wilberforce pendulum in two dimensions: one in the longitudinal and the other in torsional plain. Within each population a Kuramoto-type competition between the phases is assumed. Thus, the synchronization state of the whole system is controlled by these two types of competitions. The results of the numerical simulations show that by adding the linear cross-coupling interactions predator-prey oscillations between the two populations appear, which results in self-regulation of the system by a transfer of synchrony between the two populations. The model represents several important features of the dynamical interplay between the drift wave and zonal flow turbulence in magnetically confined plasmas, and a novel interpretation of the coupled dynamics of drift wave-zonal flow turbulence using synchronization of stochastic oscillator is discussed. (10.1103/PhysRevE.92.062930)
    DOI : 10.1103/PhysRevE.92.062930
  • 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
  • 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
  • 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
  • Intensities and spatiotemporal variability of equatorial noise emissions observed by the Cluster spacecraft
    • Nemec F.
    • Santolík O.
    • Hrbackova Z.
    • Cornilleau-Wehrlin Nicole
    Journal of Geophysical Research Space Physics, American Geophysical Union/Wiley, 2015, 120, pp.1620-1632. Equatorial noise (EN) emissions are electromagnetic waves observed in the equatorial region of the inner magnetosphere at frequencies between the proton cyclotron frequency and the lower hybrid frequency. We present the analysis of 2229 EN events identified in the Spatio-Temporal Analysis of Field Fluctuations (STAFF) experiment data of the Cluster spacecraft during the years 2001-2010. EN emissions are distinguished using the polarization analysis, and their intensity is determined based on the evaluation of the Poynting flux rather than on the evaluation of only the electric/magnetic field intensity. The intensity of EN events is analyzed as a function of the frequency, the position of the spacecraft inside/outside the plasmasphere, magnetic local time, and the geomagnetic activity. The emissions have higher frequencies and are more intense in the plasma trough than in the plasmasphere. EN events observed in the plasma trough are most intense close to the local noon, while EN events observed in the plasmasphere are nearly independent on magnetic local time (MLT). The intensity of EN events is enhanced during disturbed periods, both inside the plasmasphere and in the plasma trough. Observations of the same events by several Cluster spacecraft allow us to estimate their spatiotemporal variability. EN emissions observed in the plasmasphere do not change on the analyzed spatial scales (DeltaMLT<0.2h, Deltar<0.2 R<SUB>E</SUB>), but they change significantly on time scales of about an hour. The same appears to be the case also for EN events observed in the plasma trough, although the plasma trough dependencies are less clear. (10.1002/2014JA020814)
    DOI : 10.1002/2014JA020814
  • Magnetic Reconnection in Different Environments
    • Jackman C. M.
    • Delamere Peter A.
    • Hesse Michael
    • Aunai N.
    • Kuznetsova M. M.
    • Zenitani Seiji
    • Birn Joachim
    , 2015, 207, pp.259-267. This chapter addresses two important aspects of magnetic reconnection: time-dependent rates affected by island formation and the preferred direction of the reconnection line if merging magnetic field components are not anti-parallel. While it is widely known that magnetic reconnection facilitates mass, momentum, and energy transport in plasmas, it is illustrative to consider an analytical approach to describing the efficacy of reconnection as a transport mechanism. The chapter performs a detailed analysis of the correlation between diffusion region dimensions and reconnection rate. For this purpose, it employs open boundary condition calculations of a continuously driven reconnecting system. In summary, results indicate that the magnetic reconnection line in asymmetric systems is preferentially oriented in such a way that it bisects the direction of the asymptotic magnetic field direction on both inflow sides. This orientation is identical to the one for which the product of available magnetic energy is maximized.
  • Kinetic scale solar wind turbulence: Landau-fluid simulations and spacecraft observations
    • Sahraoui Fouad
    , 2015.
  • Gas temperature measurements in oxygen plasmas by high-resolution Two-Photon Absorption Laser-induced Fluorescence
    • Booth Jean-Paul
    • Marinov Daniil
    • Foucher Mickaël
    • Guaitella Olivier
    • Bresteau D.
    • Cabaret Louis
    • Drag Cyril
    Journal of Instrumentation, IOP Publishing, 2015, 10 (11), pp.C11003. One of the most important, and difficult to measure, parameters of laboratory discharges in molecular gases is the gas translational temperature. We propose a novel technique to measure directly, with excellent spatial and temporal resolution, the velocity distribution of ground-state atoms (oxygen atoms in this case) in plasmas from the Doppler broadening of their laser excitation spectra. The method is based on the well-known Two-Photon Laser-induced Fluorescence (TALIF) technique, but uses a specially-built pulsed tunable ultraviolet laser with very narrow bandwidth which allows the Doppler profiles to be measured with high precision. This laser consists of a pulsed Nd:YAG-pumped Ti:Sapphire ring cavity which is injection-seeded by a single-mode cw Ti:sapphire laser. The single-mode infrared output pulses are frequency quadrupled by two non-linear crystals to reach the necessary UV wavelength (226 nm, 0.2 mJ) for TALIF excitation. This technique should be applicable to a wide range of discharges, ranging from low-pressure RF plasmas for surface processing to atmospheric pressure plasmas. Results of preliminary tests on low-pressure O 2 DC discharges are presented. (10.1088/1748-0221/10/11/C11003)
    DOI : 10.1088/1748-0221/10/11/C11003
  • TALIF measurements of oxygen atom density in the afterglow of a capillary nanosecond discharge
    • Klochko A.V.
    • Lemainque J.
    • Booth Jean-Paul
    • Starikovskaia Svetlana
    Plasma Sources Science and Technology, IOP Publishing, 2015, 24 (2), pp.025010. The atomic oxygen density has been measured in the afterglow of a capillary nanosecond discharge in 2430 mbar synthetic air (N 2 &#8201;:&#8201;O 2 = 4&#8201;:&#8201;1) by the two-photon absorption laser-induced fluorescence (TALIF) technique, combined with absolute calibration by comparison with xenon TALIF. The discharge was initiated by a train of 30 ns FWHM pulses of alternating positivenegativepositive polarity, separated by 250 ns, with a train repetition frequency of 10 Hz. The amplitude of the first pulse was 10 kV in the cable. A flow of synthetic air through the tube provided complete gas renewal between pulse trains. The O-atom density measurements were made over the time interval200 ns2 µ s after the initial pulse. The gas temperature was determined by analysis of the molecular nitrogen second positive system optical emission spectrum. The influence of the gas temperature on the atom density measurements, and the reactions producing O atoms, are discussed. (10.1088/0963-0252/24/2/025010)
    DOI : 10.1088/0963-0252/24/2/025010