All Figures

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{ALFIG1.eps} \end{figure}$ Figure 1: Systematic trends of the transition rates for the 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line via the electric quadrupole (E2) mechanism along the aluminium sequence.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{ALFIG2.eps} \end{figure}$ Figure 2: Systematic trends of the transition rates for the 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line via the magnetic dipole (M1) mechanism along the aluminium sequence.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{ALFIG3.eps} \end{figure}$ Figure 3: Competition between the electric quadrupole (E2) and the magnetic dipole (M1) mechanism in the 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ transition along the aluminium sequence.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{aa3440f4.eps} \end{figure}$ Figure 4: Systematic trends for the fine-structure 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line of the aluminium and boron sequences (n = 3 and 2, respectively). For both sequences, our RQDO transition rates via the magnetic dipole (M1) mechanism are plotted versus $\xi$ , the charge on the atomic core or effective nuclear charge.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ALFIG5.eps} \end{figure}$ Figure 5: Systematic trends for the fine-structure 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line of the aluminium and boron sequences (n = 3 and 2, respectively). For both sequences, our RQDO transition rates via the electric quadrupole (E2) mechanism are plotted versus $\xi$ , the charge on the atomic core or effective nuclear charge.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{ALFIG1.eps} \end{figure}$	Figure 1: Systematic trends of the transition rates for the 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line via the electric quadrupole (E2) mechanism along the aluminium sequence.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{ALFIG2.eps} \end{figure}$	Figure 2: Systematic trends of the transition rates for the 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line via the magnetic dipole (M1) mechanism along the aluminium sequence.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{ALFIG3.eps} \end{figure}$	Figure 3: Competition between the electric quadrupole (E2) and the magnetic dipole (M1) mechanism in the 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ transition along the aluminium sequence.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{aa3440f4.eps} \end{figure}$	Figure 4: Systematic trends for the fine-structure 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line of the aluminium and boron sequences (n = 3 and 2, respectively). For both sequences, our RQDO transition rates via the magnetic dipole (M1) mechanism are plotted versus $\xi$ , the charge on the atomic core or effective nuclear charge.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ALFIG5.eps} \end{figure}$	Figure 5: Systematic trends for the fine-structure 3p $\rm {}^2P_{3/2}$ -3p $\rm {}^2P_{1/2}$ spectral line of the aluminium and boron sequences (n = 3 and 2, respectively). For both sequences, our RQDO transition rates via the electric quadrupole (E2) mechanism are plotted versus $\xi$ , the charge on the atomic core or effective nuclear charge.
Open with DEXTER