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Effects of heavy ion temperature on low-frequency kinetic Alfvén waves
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10.1063/1.3646331
/content/aip/journal/pop/18/10/10.1063/1.3646331
http://aip.metastore.ingenta.com/content/aip/journal/pop/18/10/10.1063/1.3646331
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Dependence of the normalized frequency ω/(k z A0), the normalized group velocity gx / A 0, the electric field ratio E z /E x , and the normalized electric to magnetic field ratio E x /(B y A0) on the transverse wavenumber k x λ e for different density ratios n b /n e  = 0.1 (dotted line), 0.5 (dash-dotted line), and 0.8 (solid line). Here, θ = 89°, m b /m i  = 16, γ s  = 1, q b /q i  = 1, α0 = 0.5, T i /T e  = 1, and T b /T e  = 10.

Image of FIG. 2.
FIG. 2.

Dependence of the normalized frequency ω/(k z A0), the normalized group velocity gx / A 0, the electric field ratio E z /E x , and the normalized electric to magnetic field ratio E x /(B y A0) on the heavy ion to electron temperature ratio T b /T e for α0 = 0.1 (dotted line), 1 (dash-dotted line), 5 (dashed line), and 10 (solid line). Here, k x λ e  = 0.33, T i /T e  = 1, and n b /n e  = 0.1. Other parameters are the same as those in Fig. 1.

Image of FIG. 3.
FIG. 3.

Dependence of the normalized frequency ω/(k z A0), the normalized group velocity gx / A 0, the electric field ratio E z /E x , and the normalized electric to magnetic field ratio E x /(B y A0) on the speed ratio α0 =  Te / A 0 for different density ratios n b /n e  = 0.1 (dotted line), 0.5 (dash-dotted line), and 0.8 (solid line). Here, k x λ e  = 0.33, T i /T e  = 1, and T b /T e  = 1. Other parameters are the same as those in Fig. 1.

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/content/aip/journal/pop/18/10/10.1063/1.3646331
2011-10-10
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effects of heavy ion temperature on low-frequency kinetic Alfvén waves
http://aip.metastore.ingenta.com/content/aip/journal/pop/18/10/10.1063/1.3646331
10.1063/1.3646331
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