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        conditions. The type of boundary condition at a physical domain
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        boundary is characterized by a single capital letter. It are
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        grouped in a 6-letters word with the individual letter
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        representing, from left to right, the lower-$x$ (`_C.bc[0]`),
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        upper-$x$ (`_C.bc[1]`), lower-$y$ (`_C.bc[2]`), upper-$y$
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        (`_C.bc[3]`), lower-$z$ (`_C.bc[4]`) and upper-$z$ (`_C.bc[5]`)
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        representing, from left to right, the lower-**x** (`_C.bc[0]`),
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        upper-**x** (`_C.bc[1]`), lower-**y** (`_C.bc[2]`), upper-**y**
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        (`_C.bc[3]`), lower-**z** (`_C.bc[4]`) and upper-**z** (`_C.bc[5]`)
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        domain boundary. Possible boundary condition types are
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        ($u_{i/o}$: inner/outer-domain boundary values of a variable
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        $u$):
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            $u_o=u_i$ for the perpendicular magnetic field component.
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        -   `R`: reflection-on-axis (only of relevance in cylindrical
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            geometry at the $y$-lower boundary at $R=0$ or in
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            spherical geometry at the $y$-lower/upper boundaries at
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            geometry at the **y**-lower boundary at $R=0$ or in
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            spherical geometry at the **y**-lower/upper boundaries at
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            $\theta =0,\pi$) - reflecting conditions at the geometric
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            axis. Same as M except for the azimutal magnetic field
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            component for which $u_o=-u_i$.
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        -   `C`: reflection-at-center (only of relevance in spherical
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            geometry at the $x$-lower boundary at $r=0$) - reflecting
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            geometry at the **x**-lower boundary at $r=0$) - reflecting
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            conditions at the coordinate center. Same as M except for
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            the non-radial magnetic field components for which
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            $u_o=-u_i$.
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            (pseudo-vacuum condition) for the magnetic field.
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        -   `F`: free boundary (only of relevance in cylindrical
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            geometry at the $y$-lower boundary at $R=0$ or in
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            spherical geometry at the $y$-lower/upper boundaries at
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            $\theta =0,\pi$ and $x$-lower boundary at $r=0$) -
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            geometry at the **y**-lower boundary at $R=0$ or in
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            spherical geometry at the **y**-lower/upper boundaries at
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            $\theta =0,\pi$ and **x**-lower boundary at $r=0$) -
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            'natural' boundary condition at the geometric axis. Boundary
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            values are not set explictely but are implicitly given by
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            $\pi$-shifted values. Note that when a `F`-type boundary
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