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Table 1

Definition of Local Bubble scenarios and model parameters.

Definition of Local Bubble scenarios
Names SCO SCA DCO DCA DDO DDA
Rmin Rsph Rsph RinO:=0rinner max=6$R_{{\rm{in}}}^{\rm{O}}: = 0 \leftarrow r_{{\rm{inner }}}^{{\ell _{\max }} = 6}$ ARinO${\rm{A}} \leftarrow R_{{\rm{in}}}^{\rm{O}}$ Orinner max=6${\rm{O}} \leftarrow r_{{\rm{inner }}}^{{\ell _{\max }} = 6}$ Arinner max=6${\rm{A}} \leftarrow r_{{\rm{inner }}}^{{\ell _{\max }} = 6}$
Rmax Rsph + ∆sph Rsph + ∆sph RmaxO:=RinO+Δsph$R_{\max }^O: = R_{{\rm{in}}}^{\rm{O}} + {\Delta _{{\rm{sph}}}}$ ARMO${\rm{A}} \leftarrow R_M^{\rm{O}}$ 0router max=6$0 \leftarrow r_{{\rm{outer }}}^{{\ell _{\max }} = 6}$ Arouter max=6${\rm{A}} \leftarrow r_{{\rm{outer }}}^{{\ell _{\max }} = 6}$
(xc, yc, zc) (xsph, ysph, zsph) (xcP20,ycP20,ɀcP20)$\left( {x_c^{{\rm{P}}20},y_c^{{\rm{P}}20},z_c^{{\rm{P}}20}} \right)$ (xsph, ysph, zsph) (xcP20,ycP20,ɀcP20)$\left( {x_c^{{\rm{P}}20},y_c^{{\rm{P}}20},z_c^{{\rm{P}}20}} \right)$ (xsph, ysph, zsph) (xcP20,ycP20,ɀcP20)$\left( {x_c^{{\rm{P}}20},y_c^{{\rm{P}}20},z_c^{{\rm{P}}20}} \right)$
Model parameters

xsph ysph zsph Rsph xcP20$x_c^{{\rm{P}}20}$ ycP20$y_c^{{\rm{P}}20}$ ɀcP20$y_c^{{\rm{P}}20}$ lB0${l_{{B^0}}}$ bB0${b_{{B^0}}}$
(pc) (pc) (pc) (pc) (pc) (pc) (pc) (pc) (°) (°)

–24.8 –32.6 –23.3 216.7 35 23 –34 –122 73 17

Notes. (top) Summary of the definition of the scenarios to compute the present-time magnetic field in the thick shell of the Local Bubble. (Bottom) Values for the several parameters as defined in the text. In the top table, Rmin and Rmax are the inner and outer radius of the bubble shell as measured from the explosion center in (xc, yc, zc). The left arrow (←) indicates that a surface is shifted to the coordinate system with center O := (xsph, ysph, zsph) or A :=(xcP20,ycP20,zcP20)$A: = \left( {x_c^{{\rm{P}}20},y_c^{{\rm{P}}20},z_c^{{\rm{P}}20}} \right)$, where the superscript P20 denotes the values derived in Pelgrims et al. (2020) (see their Fig. 9 and Table 1).

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