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Accueil > Pages Personnelles > E-J > Marie-Christine Firpo

Marie-Christine Firpo

CNRS research scientist.

- Invited talk, ICPP2016, Taïwan.

- Review Editor in Interdisciplinary Physics, part of the journal Frontiers in Physics.

- Member of the editorial board of the journal Discontinuity, Nonlinearity, and Complexity https://lhscientificpublishing.com/....

- Wahb Ettoumi’s thesis award : Prix Le Monde de la recherche universitaire 2014 https://www.polytechnique.edu/fr/wa... ;

- Recent works :

Magnetic reconnection : the role of chaotic magnetic field lines

 Impact of the Eulerian chaos of magnetic field lines in magnetic reconnection

http://aip.scitation.org/doi/10.106...

 Evidence and relevance of spatially chaotic magnetic field lines in MCF devices

https://doi.org/10.1088/1361-6587/aa570d

A way to detect out-of-equilibrium phase transitions :
Entropy–complexity analysis in some globally-coupled systems, Physica A 460, 162-173 (2016) http://www.sciencedirect.com/scienc....

Microtearing turbulence : magnetic braiding and disruption limit, Phys. Plasmas 22, 122511 (2015) http://scitation.aip.org/content/ai....
Abstract : A realistic reduced model involving a large poloidal spectrum of microtearing modes is used to probe the existence of some stochasticity of magnetic field lines. Stochasticity is shown to occur even for the low values of the magnetic perturbation delta_B/B devoted to magnetic turbulence that have been experimentally measured. Because the diffusion coefficient may strongly depend on the radial (or magnetic-flux) coordinate, being very low near some resonant surfaces, and because its evaluation implicitly makes a normal diffusion hypothesis, one turns to another indicator appropriate to diagnose the confinement : the mean residence time of magnetic field lines. Their computation in the microturbulence frame points to the existence of a disruption limit, namely of a critical order of magnitude of delta_B/B above which stochasticity is no longer benign yet leads to a macroscopic loss of confinement in some tens to hundred of electron toroidal excursions. Since the level of magnetic turbulence delta_B/B has been measured to grow with the plasma electron density this would also be a density limit.

Some results (partial)

On the issue of confinement in magnetic confinement devices

Turbulence may be defined, as in the theory of dynamical systems, as chaos in systems having a large number N of degrees of freedom. However, one may wonder whether the effective number of degrees of freedom behind turbulence is not much smaller, as the large N limit may regularize the dynamics. In this framework, why not consider, as a first approach to address the issue of turbulence and confinement in magnetic confinement devices, a one-and-a-half degrees of freedom description as a minimal skeleton for chaos ? Such a system is naturally given by the equations for the magnetic field lines. So doing, one addresses the issue of plasma confinement through the deeper, more fondamental issue of the confinement of magnetic field lines.

Some related publications :

- L. Nasi and M.-C. Firpo, Enhanced confinement with increased extent of the low magnetic shear region in tokamak plasmas, Plasma Physics and Controlled Fusion 51 045006, 2009.http://iopscience.iop.org/0741-3335...

- M.-C. Firpo and D. Constantinescu, Study of the interplay between magnetic shear and resonances
using Hamiltonian models for the magnetic field lines
, Physics of Plasmas 18 032506, 2011.http://pop.aip.org/resource/1/phpae...

- D. Constantinescu and M.-C. Firpo, Modifying locally the safety profile to improve the confinement of magnetic field lines in tokamak plasmas, Nucl. Fusion 52 054006, 2012. http://iopscience.iop.org/0029-5515...

Early nonlinear regime of the m=1 internal mode

The development into the nonlinear regime of the m=1 resistive mode, whose destabilization governs the sawteeth phenomenon of small tokamaks, is predicted. This problem is addressed by realizing that two small parameters are involved : one is the resistivity, assumed to be constant in time, the other one is the mode amplitude A, which is time dependent. An amplitude expansion is derived. The entrance into the nonlinear regime is shown to proceed through successive phases, separated by thresholds in amplitude given by power laws in the resistivity. This happens to be a general feature in the dynamics of magnetic reconnection, as observed in experiments or numerical simulations.

Some related publications :

- M.-C. Firpo and B. Coppi, Dynamical Analysis of the Nonlinear Growth of the m=n=1 Resistive Internal Mode, Phys. Rev. Lett. 90, 095003 (2003). http://prl.aps.org/abstract/PRL/v90...

- M.-C. Firpo, Onset of the nonlinear regime and finite-resistivity effects for the resistive kink instability, Phys. Plasmas. 11, 970 (2004).http://pop.aip.org/resource/1/phpae...

A statistical mechanics viewpoint on nonlinear Landau damping

Wave-particle interactions are an ubiquitous phenomenon in hot plasmas. In the electrostatic approximation, it is possible to write down a reduced Hamiltonian description of the interaction between Langmuir waves and resonant particles [1].

The question of the long-time fate of the electric field in the case of initial conditions subject to Landau damping has been much debated. Under the ergodic hypothesis, this may be answered through an equilibrium statistical mechanics approach of the finite-dimensional wave-particle Hamiltonian model.

In the case of damping of a single Langmuir wave, O’Neil’s threshold, that separates nonzero time-asymptotic wave amplitude states from zero ones, is associated to a second order phase transition [2]. In the general case of a continuum of waves, in which the ergodic hypothesis is the most likely to be satisfied, the wave spectrum is predicted to collapse towards small wavelengths together with the escape of initially resonant particles towards low bulk plasma thermal speeds. This study [3] reveals the fundamental discrepancy between the long-time dynamics of single waves, that can support finite amplitude steady states, and of wave spectra, that cannot.

[1] Y. Elskens and D. F. Escande, Microscopic Dynamics of Plasmas and Chaos (IOP, Bristol, 2002).

[2] M.-C. Firpo and Y. Elskens,
Phase Transition in the Collisionless Damping Regime for Wave-Particle Interaction
, Phys. Rev. Lett. 84, 3318 (2000).http://prl.aps.org/abstract/PRL/v84...

[3] M.-C. Firpo, F. Leyvraz and G. Attuel, Equilibrium statistical mechanics for single waves and wave spectra in Langmuir wave-particle interaction, Phys. Plasmas 13, 122302 (2006).http://pop.aip.org/resource/1/phpae...

Beam-plasma interactions for fast ignition applications

Inertial confinement fusion schemes commonly involve in their final stage the interaction between some highly energetic particle beams and a dense plasma target. This is in particular valid for the Fast Ignition Scenario (FIS) where some laser-produced relativistic electron beam would eventually propagate into the dense plasma where it would be stopped. In this respect, microscopic turbulence in beam-plasma systems is one of the main potentially deleterious effects since it may prevent the conditions for burn to be met by broadening the phase area where particles deposit their energy. Within the FIS framework, a strong research effort has thus been put recently on the interaction of a relativistic electron beam with a plasma with a focus on beam filamentation instability, that is microscopic in the transverse direction.
Linear theory of the beam/return plasma equilibrium setting, done without any restriction on the wave vector orientation, reveals that filamentation is mainly triggered by an oblique mode belonging to the two-stream/filamentation branch.

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