id	author	title	date	pages	extension	mime	words	sentence	flesch	summary	cache	txt
ap-1751	Horký, Miroslav	Instability Growth Rate Dependence on Input Parameters During the Beam–Target Plasma Interaction	2013	5	.pdf	application/pdf	2544	154	69	−Ω2 1ω 2 c1 − Ω1ω 2 c1k(G3) + ( ω2 c1k 2 c2 s1 + ω2 c1ω 2 p1 ) (G2)2 ] · [ Ω 4 2 + iΩ2 2ωc2ku2(G1)−Ω2 2 ( c2 s2k 2 + 1 ) −Ω2 2ω 2 c2 − Ω2ω 2 c2ku2(G3) + ( ω2 c2k 2 c2 s2 + ω2 c2 ) (G2)2 ] − [ ω2 p1 ( Ω 2 1 − ω2 c1(G2)2 )] · [ Ω 2 2 − ω2 c2(G2)2 ] = 0, (5) where we denoted G1 = (cos θB sinϕ sin θk), G2 = (cosϕ sin θk sin θB + cos θk cos θB), G3 = (cos2 θB cosϕ sin θk − cos θB cos θk sin θB), Ω1 = ω − k cosϕ sin θk, Ω2 = ω − ku2 cosϕ sin θk. [ iF (0) α · eB mα + ( c2 sαk 2 + ω2 pα ) k · eB k2 ]} − 2∏ α=1 ω2 pα k2 [ Ω2 αk 2 − ω2 cα (eB · k)2 ] = 0, (3) where Ωα = ω − k · u(0) α , (4) ωcα is the cyclotron frequency, F(0) α is the Lorentz magnetic force, eB is the unit vector in the direc- tion of magnetic field and csα is the sound velocity.	cache/ap-1751.pdf	txt/ap-1751.txt