2014
			
	    
	
	
    Covariant formulation of spatially non-symmetric kinetic equilibria in magnetized astrophysical plasmas
CREMASCHINI, Claudio; Zdeněk STUCHLÍK and Massimo TESSAROTTOBasic information
Original name
Covariant formulation of spatially non-symmetric kinetic equilibria in magnetized astrophysical plasmas
	Authors
CREMASCHINI, Claudio; Zdeněk STUCHLÍK and Massimo TESSAROTTO
			Edition
 PHYSICS OF PLASMAS, US - Spojené státy americké, 2014, 1070-664X
			Other information
Language
English
		Type of outcome
Article in a journal
		Field of Study
10305 Fluids and plasma physics
		Confidentiality degree
is not subject to a state or trade secret
		References:
Impact factor
Impact factor: 2.142
			Organization unit
Faculty of Philosophy and Science in Opava
			UT WoS
000337107200046
		EID Scopus
2-s2.0-84900477222
		Keywords in English
astrophysical plasmas; kinetic equilibrium; compact objects; gravitational field
		Tags
Tags
International impact, Reviewed
		Links
GB14-37086G, research and development project. GP14-07753P, research and development project. 
			
				
				Changed: 26/1/2021 17:14, Mgr. Pavlína Jalůvková
				
		Abstract
In the original language
Astrophysical plasmas in the surrounding of compact objects and subject to intense gravitational and electromagnetic fields are believed to give rise to relativistic regimes. Theoretical and observational evidences suggest that magnetized plasmas of thistype are collisionless and can persist for long times (e.g., with respect to a distant observer, coordinate, time), while exhibiting geometrical structures characterized by the absence of well-defined spatial symmetries. In this paper, the problem is posed whether such configurations can correspond to some kind of kinetic equilibrium. The issue is addressed from a theoretical perspective in the framework of a covariant Vlasov statistical description, which relies on the method of invariants. For this purpose, a systematic covariant variational formulation of gyrokinetic theory is developed, which holds without requiring any symmetry condition on the background fields. As a result, an asymptotic representation of the relativistic partic