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Statements

Subject Item
n2:RIV%2F68378289%3A_____%2F12%3A00373513%21RIV12-AV0-68378289
rdf:type
skos:Concept n13:Vysledek
rdfs:seeAlso
http://link.aps.org/doi/10.1103/PhysRevLett.108.025002
dcterms:description
Whistler wave trains are observed in the foot region of high Mach number quasiperpendicular shocks. The waves are oblique with respect to the ambient magnetic field as well as the shock normal. The Poynting flux of the waves is directed upstream in the shock normal frame starting from the ramp of the shock. This suggests that the waves are an integral part of the shock structure with the dispersive shock as the source of the waves. These observations lead to the conclusion that the shock ramp structure of supercritical high Mach number shocks is formed as a balance of dispersion and nonlinearity. Whistler wave trains are observed in the foot region of high Mach number quasiperpendicular shocks. The waves are oblique with respect to the ambient magnetic field as well as the shock normal. The Poynting flux of the waves is directed upstream in the shock normal frame starting from the ramp of the shock. This suggests that the waves are an integral part of the shock structure with the dispersive shock as the source of the waves. These observations lead to the conclusion that the shock ramp structure of supercritical high Mach number shocks is formed as a balance of dispersion and nonlinearity.
dcterms:title
Dispersive Nature of High Mach Number Collisionless Plasma Shocks: Poynting Flux of Oblique Whistler Waves Dispersive Nature of High Mach Number Collisionless Plasma Shocks: Poynting Flux of Oblique Whistler Waves
skos:prefLabel
Dispersive Nature of High Mach Number Collisionless Plasma Shocks: Poynting Flux of Oblique Whistler Waves Dispersive Nature of High Mach Number Collisionless Plasma Shocks: Poynting Flux of Oblique Whistler Waves
skos:notation
RIV/68378289:_____/12:00373513!RIV12-AV0-68378289
n13:predkladatel
n14:ico%3A68378289
n3:aktivita
n20:Z
n3:aktivity
Z(AV0Z30420517)
n3:cisloPeriodika
2
n3:dodaniDat
n6:2012
n3:domaciTvurceVysledku
n18:2700514
n3:druhVysledku
n5:J
n3:duvernostUdaju
n15:S
n3:entitaPredkladatele
n16:predkladatel
n3:idSjednocenehoVysledku
131539
n3:idVysledku
RIV/68378289:_____/12:00373513
n3:jazykVysledku
n8:eng
n3:klicovaSlova
shock waves and discontinuities; bow shock; plasma waves
n3:klicoveSlovo
n4:bow%20shock n4:shock%20waves%20and%20discontinuities n4:plasma%20waves
n3:kodStatuVydavatele
US - Spojené státy americké
n3:kontrolniKodProRIV
[62BFD23A9062]
n3:nazevZdroje
Physical Review Letters
n3:obor
n17:BL
n3:pocetDomacichTvurcuVysledku
1
n3:pocetTvurcuVysledku
6
n3:rokUplatneniVysledku
n6:2012
n3:svazekPeriodika
108
n3:tvurceVysledku
Krasnoselskikh, V. Mozer, F. Sundkvist, D. Schwartz, S. J. Souček, Jan Bale, S. D.
n3:wos
000298991400014
n3:zamer
n19:AV0Z30420517
s:issn
0031-9007
s:numberOfPages
4
n9:doi
10.1103/PhysRevLett.108.025002