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Effect of magnetic field on the wave dispersion relation in three-dimensional dusty plasma crystals
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10.1063/1.4737600
/content/aip/journal/pop/19/7/10.1063/1.4737600
http://aip.metastore.ingenta.com/content/aip/journal/pop/19/7/10.1063/1.4737600
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Sketch diagram of characteristic directions.

Image of FIG. 2.
FIG. 2.

Dependence of the dispersion relation on the magnetic field for the OM (solid line), HPM (dashed line), and LPM (dotted line) when the wave vector is parallel to the (1,0,0) direction and the magnetic field is perpendicular to with the screening parameter . Black lines are for and red lines are for . (a1) and (b1) are the dispersion relations and the mode mixing parameters P in the bcc lattice, respectively. (a2) and (b2) are the dispersion relations and the mode mixing parameters P in the fcc lattice, respectively.

Image of FIG. 3.
FIG. 3.

Dependence of the dispersion relation on the magnetic field for the OM (solid line), HPM (dashed line), and LPM (dotted line) when the wave vector is parallel to the (1,1,1) direction and the magnetic field is perpendicular to with the screening parameter . Black lines are for and red lines are for . (a1) and (b1) are the dispersion relations and the mode mixing parameters P in the bcc lattice, respectively. (a2) and (b2) are the dispersion relations and the mode mixing parameters P in the fcc lattice, respectively.

Image of FIG. 4.
FIG. 4.

Dependence of the dispersion relation on the magnetic field for the OM (solid line), HPM (dashed line), and LPM (dotted line) when the wave vector is parallel to (1,1,0) direction, and the magnetic field is parallel to (0,0,1) direction with the screening parameter . Black lines are for and red lines are for . (a1) and (b1) are the dispersion relations and the mode mixing parameters P in the bcc lattice, respectively. (a2) and (b2) are the dispersion relations and the mode mixing parameters P in the fcc lattice, respectively.

Image of FIG. 5.
FIG. 5.

Dependence of the dispersion relation on the magnetic field for the OM (solid line), HPM (dashed line), and LPM (dotted line) when the wave vector is parallel to (1,1,0) direction, and the magnetic field is parallel to (1,−1,0) direction with the screening parameter . Black lines are for and red lines are for . (a1) and (b1) are the dispersion relations and the mode mixing parameters P in the bcc lattice, respectively. (a2) and (b2) are the dispersion relations and the mode mixing parameters P in the fcc lattice, respectively.

Image of FIG. 6.
FIG. 6.

Dependence of the dispersion relation on the magnetic field for the OM (solid line), HPM (dashed line), and LPM (dotted line) when the wave vector is parallel to the (1,0,0) direction and the magnetic field is parallel to with the screening parameter . Black lines are for and red lines are for . (a1) and (b1) are the dispersion relations and the mode mixing parameters P in the bcc lattice, respectively. (a2) and (b2) are the dispersion relations and the mode mixing parameters P in the fcc lattice, respectively.

Image of FIG. 7.
FIG. 7.

The wave frequency and the mode mixing parameters P as a function of the cyclotron frequency for the OM (solid line), HPM (dashed line), and LPM (dotted line) when the wave vector is parallel to the (1,0,0) direction andthe magnetic field is parallel to with the screening parameter and the wavenumber .

Image of FIG. 8.
FIG. 8.

The acoustic velocity of HPM as a function of for the screening parameter (solid line), (dashed line), and (dotted line) when the wave vector is parallel to the (1,0,0) direction.

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/content/aip/journal/pop/19/7/10.1063/1.4737600
2012-07-18
2014-04-25
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effect of magnetic field on the wave dispersion relation in three-dimensional dusty plasma crystals
http://aip.metastore.ingenta.com/content/aip/journal/pop/19/7/10.1063/1.4737600
10.1063/1.4737600
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