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$\begin{figure} \par\includegraphics[width=6cm,angle=270]{8530fig1.eps}\end{figure}$ Figure 1: Spin polarisation for temperature and electron chemical potential scaled by the magnetic field.
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In the text

$\begin{figure} \par\includegraphics[width=6cm,angle=270]{8530fig2.eps}\end{figure}$ Figure 2: Constraint to fully polarise the electron spin for different magnetic fields in dependence on the temperature and the electron chemical potential.
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In the text

$\begin{figure} \par\mbox{\subfigure{\includegraphics[width=8cm]{8530fig3a.eps} } \subfigure{\includegraphics[width=8cm]{8530fig3b.eps} }} \end{figure}$ Figure 3: Comparison of the numerical and analytical results for the electron spin polarisation. a) gives the polarisation for T=0 and b) shows the case of $\mu , m\ll T\ll \sqrt {2eB}$ . The difference between the numerical and the analytical results in the latter is max. 10%.
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In the text

$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig4.eps}\end{figure}$ Figure 4: Neutrino mean free paths in quark matter and neutron matter for $E_\nu =3.15T$ , $\mu _{\rm q}=400$ MeV, $\alpha _{\rm s}=0.5$ , $n_{\rm n}=n_0$ and $\mu _{\rm e}$ =10 MeV.
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In the text

$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig5.eps} \end{figure}$ Figure 5: Neutrino mean free paths in quark matter and neutron matter for $E_\nu =3T$ , $\mu _{\rm q}=400$ MeV, $\alpha _{\rm s}=0.5$ , $n_{\rm n}=0.16$ fm^-3 and $\mu _{\rm e}=10$ MeV with kick velocities for $M_{\rm ns}=1.4~M_\odot$ and full electron spin polarisation.
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In the text

$\begin{figure} \par\mbox{\subfigure[Strong coupling constant $\alpha_{\rm s}=0.3... ...\sim T$ .]{\includegraphics[width=6cm, angle=270]{8530fig6d.eps} }} \end{figure}$ Figure 6: Kick velocities and neutrino mean free paths in quark matter and neutron matter as in Fig. 5.
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In the text

$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig7.eps}\end{figure}$ Figure 7: Kick velocities and neutrino mean free path in quark matter for the CFL quark phase with $\alpha _{\rm s}=0.5$ , $\mu _{\rm q}=450$ MeV, $\mu _{\rm e}=100$ MeV, and $\Delta =100$ MeV.
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In the text

$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig8.eps}\end{figure}$ Figure 8: Kick velocities due to a phase transition from ungapped to paired quark matter with $\mu _{\rm q}=450$ MeV and $\Delta = 20$ MeV. Neutrino mean free paths are plotted assuming an electron chemical potential of 10 MeV and normal nuclear matter density for hadronic matter. The neutrino energy is $E_\nu = \Delta ^2/\mu _{\rm q}$ . For the quark phase, gap suppression is also taken into account (solid line). In addition, the neutrino mean free path in normal quark matter is plotted (dotted line).
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In the text

$\begin{figure} \par\includegraphics[width=6cm,angle=270]{8530fig1.eps}\end{figure}$	Figure 1: Spin polarisation for temperature and electron chemical potential scaled by the magnetic field.
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$\begin{figure} \par\includegraphics[width=6cm,angle=270]{8530fig2.eps}\end{figure}$	Figure 2: Constraint to fully polarise the electron spin for different magnetic fields in dependence on the temperature and the electron chemical potential.
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$\begin{figure} \par\mbox{\subfigure{\includegraphics[width=8cm]{8530fig3a.eps} } \subfigure{\includegraphics[width=8cm]{8530fig3b.eps} }} \end{figure}$	Figure 3: Comparison of the numerical and analytical results for the electron spin polarisation. a) gives the polarisation for T=0 and b) shows the case of $\mu , m\ll T\ll \sqrt {2eB}$ . The difference between the numerical and the analytical results in the latter is max. 10%.
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$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig4.eps}\end{figure}$	Figure 4: Neutrino mean free paths in quark matter and neutron matter for $E_\nu =3.15T$ , $\mu _{\rm q}=400$ MeV, $\alpha _{\rm s}=0.5$ , $n_{\rm n}=n_0$ and $\mu _{\rm e}$ =10 MeV.
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$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig5.eps} \end{figure}$	Figure 5: Neutrino mean free paths in quark matter and neutron matter for $E_\nu =3T$ , $\mu _{\rm q}=400$ MeV, $\alpha _{\rm s}=0.5$ , $n_{\rm n}=0.16$ fm^-3 and $\mu _{\rm e}=10$ MeV with kick velocities for $M_{\rm ns}=1.4~M_\odot$ and full electron spin polarisation.
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$\begin{figure} \par\mbox{\subfigure[Strong coupling constant $\alpha_{\rm s}=0.3... ...\sim T$ .]{\includegraphics[width=6cm, angle=270]{8530fig6d.eps} }} \end{figure}$	Figure 6: Kick velocities and neutrino mean free paths in quark matter and neutron matter as in Fig. 5.
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$\begin{figure} \par\includegraphics[width=6cm, angle=270]{8530fig7.eps}\end{figure}$	Figure 7: Kick velocities and neutrino mean free path in quark matter for the CFL quark phase with $\alpha _{\rm s}=0.5$ , $\mu _{\rm q}=450$ MeV, $\mu _{\rm e}=100$ MeV, and $\Delta =100$ MeV.
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