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Kinetic theory of linear fluctuations in magnetized and unmagnetized collisionfree plasmas

Subject Area Optics, Quantum Optics and Physics of Atoms, Molecules and Plasmas
Astrophysics and Astronomy
Term from 2015 to 2019
Project identifier Deutsche Forschungsgemeinschaft (DFG) - Project number 275578165
 
Final Report Year 2019

Final Report Abstract

Fluctuations are a generic feature of all plasmas due to the finite random velocities of the plasma particles. The two major scientific objectives of this project were (i) the extension of the kinetic plasma fluctuation theory in unmagnetized plasmas calculating in particular the associated density and velocity fluctuation spectra of weakly propagating and weakly amplified/damped modes (collective and non-collective modes), and (ii) the development of the general kinetic fluctuation theory for magnetized plasmas using the existing fluctuation theory of unmagnetized plasmas. In both cases the classical linear fluctuation theory, based on the coupled Klimontovich-Maxwell equations, is developed with two important generalizations: no restrictions on the generally complex frequency ω = ωR + ıΓ of the fluctuations are made, and the calculations use the correct relativistic relation p = mγp v between plasma particle momentum p and velocity v with the Lorentz factor γp = √ 1 + (p/mc)2. The intergalactic medium (IGM) at high redshifts is the most prominent unmagnetized fully-ionized cosmic plasma, i.e. it is not permeated by an ordered magnetic (and/or electric) field. However, the IGM contains electric and magnetic field fluctuations, which play an important role in the understanding of the origin of cosmic magnetic fields. Especially seed magnetic fields are needed for later amplification by possible kinetic instabilities from anisotropic plasma particle distribution functions, MHD instabilities and/or the MHD dynamo process. For two phases of the early universe IGM, the reionization era at redshift z≈20 and the pamyprepanne era at redshifts 1.4 · 10^12 ≥ z ≥ 6 · 10^9 , the properties of the fluctuations are quantatively calculated. During the pamyprepanne random electric and magnetic fields in the form of aperiodic fluctuations with very high tera-Gauss strengths |δB| and |δE| were generated by the relativistic electron-positron pairs on spatial scales greater than L ≈ 10^−10 cm with 100 percent volume filling factor. These aperiodic fluctuations have a substantial energy density though about three orders of magnitude smaller than the superluminal photon energy density, so that the aperiodic fluctuations have a negligible influence on the radiation-driven cosmological evolution during the pamyprepanne. For magnetized plasmas the rigorous relativistic kinetic theory to calculate linear electromagnetic fluctuations in magnetized plasmas was developed. This theory allows us to calculate the resulting spontaneous emission coefficients and damping or growth rates for any orientation angle of the wave vector with respect to the ordered magnetic field, although the details are involved.

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