All Figures

$\begin{figure} \par\includegraphics[width=7cm]{3885fig1} \end{figure}$ Figure 1: DA193 at 5 GHz, the restoring beam is $3.7\times 1.4$ mas in PA $21.0^{\circ }$ , the contours are total intensity with 34 mJy/beam times -2, -1, 1, 2, 5, 10, 20, 40, 80, and the peak of 3433 mJy/beam. The overlay in grey is linearly polarized intensity, with the peak of 56 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig2} \end{figure}$ Figure 2: Linear polarization map of DA193 with polarization angle superimposed at 5 GHz, the restoring beam is $2.8\times 1.9$ mas in PA $32.5^{\circ }$ , the contours are 20 mJy/beam times -2, -1, 1, 2, with the peak of 56 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig3} \end{figure}$ Figure 3: 0554-026 at 5 GHz, the restoring beam is $3.8\times 2.5$ mas in PA $-5.8^{\circ }$ , the contours are 1.5 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, with the peak of 71 mJy/beam. The electric vectors of possible polarizations are superimposed.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig4} \end{figure}$ Figure 4: 0914+114 at 5 GHz, the restoring beam is $4.7\times 2.9$ mas in PA $-1.5^{\circ }$ , the contours are 1.6 mJy/beam times -2, 1, 2, 4, 8, with the peak of 28 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig5} \end{figure}$ Figure 5: Component spectra of source 0914+114 from the VLBI data at 2.3, 5.0, and 8.4 GHz, where flux of component C at 8.4 GHz is $\leq$ 1 mJy.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig6} \end{figure}$ Figure 6: 1133+432 at 5 GHz, the restoring beam is $2.2\times 2.0$ mas in PA $51^{\circ }$ , the contours are 1.5 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 134 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig7} \end{figure}$ Figure 7: Component spectra of source 1133+432 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig8} \end{figure}$ Figure 8: 1333+589 at 5 GHz, the restoring beam is $3.2\times 3.0$ mas in PA $-87^{\circ }$ , the contours are 10 mJy/beam times -2, 1, 2, 4, 8, 16, with the peak of 290 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=6.8cm]{3885fig9} \end{figure}$ Figure 9: Component spectra of source 1333+589 from the VLBI data at 1.6, 2.3, 5.0, and 8.4 GHz.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg10} \end{figure}$ Figure 10: OQ208 at 5 GHz, the restoring beam is $3.7\times 2.6$ mas in PA $0^{\circ }$ , the contours are 20 mJy/beam times -2, 1, 2, 4, 8, 16, 32, 64, with the peak of 1749 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg11}\end{figure}$ Figure 11: 1433-040 at 5 GHz, the restoring beam is $3.6\times 2.5$ mas in PA $-8.6^{\circ }$ , the contours are total intensity with 2.0 mJy/beam times -2, 1, 2, 4, 8, 16, 32, 64, 90, and the peak of 84.2 mJy/beam. The overlay in grey is linearly polarized intensity, with the peak of 3.8 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg12} \end{figure}$ Figure 12: Linear polarization map of 1433-040 with polarization angle superimposed at 5 GHz, the restoring beam is $5.0\times 3.4$ mas in PA $1.8^{\circ }$ , the contours are 0.5 mJy/beam times -2, -1, 1, 2, 4, with the peak of 3.8 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg13} \end{figure}$ Figure 13: 1509+054 at 5 GHz using uniform weighting with an AIPS robust parameter of 1, the restoring beam is $4.2\times 2.94$ mas in PA $-3.3^{\circ }$ , the contours are 4 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 407 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg14} \end{figure}$ Figure 14: 1509+054 at 5 GHz using uniform weighting with an AIPS robust parameter of -2, the restoring beam is $3.6\times 1.2$ mas in PA $5.2^{\circ }$ , the contours are 6 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, with the peak of 325 mJy/beam. The electric vectors of possible polarizations are superimposed.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg15} \end{figure}$ Figure 15: 1518+046 at 5 GHz, the restoring beam is $4.4\times 3.0$ mas in PA $-0.3^{\circ }$ , the contours are 4 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 276 mJy/beam. The electric vectors of possible polarizations are superimposed.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg16} \end{figure}$ Figure 16: 1751+278 at 5 GHz, the restoring beam is $4.1\times 3.0$ mas in PA $1.8^{\circ }$ , the contours are 2.0 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 170 mJy/beam. The electric vectors of possible polarizations are superimposed.
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In the text

$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg17} \end{figure}$ Figure 17: 1824+271 at 5 GHz, the restoring beam is $4.6\times 3.5$ mas in PA $1.7^{\circ }$ , the contours are 0.9 mJy/beam times -2, 1, 2, 4, 8, 16, 32, with the peak of 50 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fg18} \end{figure}$ Figure 18: Component spectra of source 1824+271 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fg19} \end{figure}$ Figure 19: 2121-014 at 5 GHz, the restoring beam is $4.7\times 3.4$ mas in PA $4.9^{\circ }$ , the contours are 2 mJy/beam times -2, 1, 2, 4, 8, 16, 32, with the peak of 107 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fg20} \end{figure}$ Figure 20: Component spectra of source 2121-014 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fg21} \end{figure}$ Figure 21: 2322-040 at 5 GHz, the restoring beam is $4.0\times 2.3$ mas in PA $-7.6^{\circ }$ , the contours are 6 mJy/beam times -2, 1, 2, 4, 8, 16, 32, with the peak of 299 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fg22} \end{figure}$ Figure 22: Component spectra of source 2322-040 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fg23} \end{figure}$ Figure 23: 2323+790 at 5 GHz, the restoring beam is $3.8\times 3.1$ mas in PA $-1.6^{\circ }$ , the contours are 2 mJy/beam times -2, 1, 2, 4, 8, 16, 32, 64, with the peak of 184 mJy/beam.
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In the text

$\begin{figure} \par\includegraphics[width=7cm]{3885fig1} \end{figure}$	Figure 1: DA193 at 5 GHz, the restoring beam is $3.7\times 1.4$ mas in PA $21.0^{\circ }$ , the contours are total intensity with 34 mJy/beam times -2, -1, 1, 2, 5, 10, 20, 40, 80, and the peak of 3433 mJy/beam. The overlay in grey is linearly polarized intensity, with the peak of 56 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig2} \end{figure}$	Figure 2: Linear polarization map of DA193 with polarization angle superimposed at 5 GHz, the restoring beam is $2.8\times 1.9$ mas in PA $32.5^{\circ }$ , the contours are 20 mJy/beam times -2, -1, 1, 2, with the peak of 56 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig3} \end{figure}$	Figure 3: 0554-026 at 5 GHz, the restoring beam is $3.8\times 2.5$ mas in PA $-5.8^{\circ }$ , the contours are 1.5 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, with the peak of 71 mJy/beam. The electric vectors of possible polarizations are superimposed.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig4} \end{figure}$	Figure 4: 0914+114 at 5 GHz, the restoring beam is $4.7\times 2.9$ mas in PA $-1.5^{\circ }$ , the contours are 1.6 mJy/beam times -2, 1, 2, 4, 8, with the peak of 28 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig5} \end{figure}$	Figure 5: Component spectra of source 0914+114 from the VLBI data at 2.3, 5.0, and 8.4 GHz, where flux of component C at 8.4 GHz is $\leq$ 1 mJy.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig6} \end{figure}$	Figure 6: 1133+432 at 5 GHz, the restoring beam is $2.2\times 2.0$ mas in PA $51^{\circ }$ , the contours are 1.5 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 134 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig7} \end{figure}$	Figure 7: Component spectra of source 1133+432 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fig8} \end{figure}$	Figure 8: 1333+589 at 5 GHz, the restoring beam is $3.2\times 3.0$ mas in PA $-87^{\circ }$ , the contours are 10 mJy/beam times -2, 1, 2, 4, 8, 16, with the peak of 290 mJy/beam.
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$\begin{figure} \par\includegraphics[width=6.8cm]{3885fig9} \end{figure}$	Figure 9: Component spectra of source 1333+589 from the VLBI data at 1.6, 2.3, 5.0, and 8.4 GHz.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg10} \end{figure}$	Figure 10: OQ208 at 5 GHz, the restoring beam is $3.7\times 2.6$ mas in PA $0^{\circ }$ , the contours are 20 mJy/beam times -2, 1, 2, 4, 8, 16, 32, 64, with the peak of 1749 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg11}\end{figure}$	Figure 11: 1433-040 at 5 GHz, the restoring beam is $3.6\times 2.5$ mas in PA $-8.6^{\circ }$ , the contours are total intensity with 2.0 mJy/beam times -2, 1, 2, 4, 8, 16, 32, 64, 90, and the peak of 84.2 mJy/beam. The overlay in grey is linearly polarized intensity, with the peak of 3.8 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg12} \end{figure}$	Figure 12: Linear polarization map of 1433-040 with polarization angle superimposed at 5 GHz, the restoring beam is $5.0\times 3.4$ mas in PA $1.8^{\circ }$ , the contours are 0.5 mJy/beam times -2, -1, 1, 2, 4, with the peak of 3.8 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg13} \end{figure}$	Figure 13: 1509+054 at 5 GHz using uniform weighting with an AIPS robust parameter of 1, the restoring beam is $4.2\times 2.94$ mas in PA $-3.3^{\circ }$ , the contours are 4 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 407 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg14} \end{figure}$	Figure 14: 1509+054 at 5 GHz using uniform weighting with an AIPS robust parameter of -2, the restoring beam is $3.6\times 1.2$ mas in PA $5.2^{\circ }$ , the contours are 6 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, with the peak of 325 mJy/beam. The electric vectors of possible polarizations are superimposed.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg15} \end{figure}$	Figure 15: 1518+046 at 5 GHz, the restoring beam is $4.4\times 3.0$ mas in PA $-0.3^{\circ }$ , the contours are 4 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 276 mJy/beam. The electric vectors of possible polarizations are superimposed.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg16} \end{figure}$	Figure 16: 1751+278 at 5 GHz, the restoring beam is $4.1\times 3.0$ mas in PA $1.8^{\circ }$ , the contours are 2.0 mJy/beam times -2, -1, 1, 2, 4, 8, 16, 32, 64, with the peak of 170 mJy/beam. The electric vectors of possible polarizations are superimposed.
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$\begin{figure} \par\includegraphics[width=7.2cm]{3885fg17} \end{figure}$	Figure 17: 1824+271 at 5 GHz, the restoring beam is $4.6\times 3.5$ mas in PA $1.7^{\circ }$ , the contours are 0.9 mJy/beam times -2, 1, 2, 4, 8, 16, 32, with the peak of 50 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fg18} \end{figure}$	Figure 18: Component spectra of source 1824+271 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fg19} \end{figure}$	Figure 19: 2121-014 at 5 GHz, the restoring beam is $4.7\times 3.4$ mas in PA $4.9^{\circ }$ , the contours are 2 mJy/beam times -2, 1, 2, 4, 8, 16, 32, with the peak of 107 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fg20} \end{figure}$	Figure 20: Component spectra of source 2121-014 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fg21} \end{figure}$	Figure 21: 2322-040 at 5 GHz, the restoring beam is $4.0\times 2.3$ mas in PA $-7.6^{\circ }$ , the contours are 6 mJy/beam times -2, 1, 2, 4, 8, 16, 32, with the peak of 299 mJy/beam.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fg22} \end{figure}$	Figure 22: Component spectra of source 2322-040 from the VLBI data at 2.3, 5.0, and 8.4 GHz.
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$\begin{figure} \par\includegraphics[width=7cm]{3885fg23} \end{figure}$	Figure 23: 2323+790 at 5 GHz, the restoring beam is $3.8\times 3.1$ mas in PA $-1.6^{\circ }$ , the contours are 2 mJy/beam times -2, 1, 2, 4, 8, 16, 32, 64, with the peak of 184 mJy/beam.
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