All Figures

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{hanasz-3344-f1.eps} \end{figure}$ Figure 1: Geometry of the magnetic field in the vicinity of the current sheet before the onset of reconnection. The current sheet corresponding to the contact discontinuity of magnetic field is coplanar with the xz plane. The two magnetic field vectors inclined with respect to the x-axis represent two magnetic field lines on both sides of the current sheet.
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In the text

$\begin{figure} \par\includegraphics[width=7.9cm,clip]{hanasz-3344-f2.ps}\end{figure}$ Figure 2: Parameter space for quadratic waves. Numbering of different regions follows the list following conditions (1) and (2). An additional region on the left of the figure results form the upper limit on the guiding field B_z.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{hanasz-3344-f1.eps} \end{figure}$	Figure 1: Geometry of the magnetic field in the vicinity of the current sheet before the onset of reconnection. The current sheet corresponding to the contact discontinuity of magnetic field is coplanar with the xz plane. The two magnetic field vectors inclined with respect to the x-axis represent two magnetic field lines on both sides of the current sheet.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=7.9cm,clip]{hanasz-3344-f2.ps}\end{figure}$	Figure 2: Parameter space for quadratic waves. Numbering of different regions follows the list following conditions (1) and (2). An additional region on the left of the figure results form the upper limit on the guiding field B_z.
Open with DEXTER