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   <subfield code="a">A well-balanced and asymptotic-preserving scheme for the one-dimensional linear Dirac equation</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Laurent Gosse]</subfield>
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   <subfield code="a">The numerical approximation of one-dimensional relativistic Dirac wave equations is considered within the recent framework consisting in deriving local scattering matrices at each interface of the uniform Cartesian computational grid. For a Courant number equal to unity, it is rigorously shown that such a discretization preserves exactly the $$L^2$$ L 2 norm despite being explicit in time. This construction is well-suited for particles for which the reference velocity is of the order of $$c$$ c , the speed of light. Moreover, when $$c$$ c diverges, that is to say, for slow particles (the characteristic scale of the motion is non-relativistic), Dirac equations are naturally written so as to let a &quot;diffusive limit” emerge numerically, like for discrete 2-velocity kinetic models. It is shown that an asymptotic-preserving scheme can be deduced from the aforementioned well-balanced one, with the following properties: it yields unconditionally a classical Schrödinger equation for free particles, but it handles the more intricate case with an external potential only conditionally (the grid should be such that $$c \Delta x\rightarrow 0$$ c Δ x → 0 ). Such a stringent restriction on the computational grid can be circumvented easily in order to derive a seemingly original Schrödinger scheme still containing tiny relativistic features. Numerical tests (on both linear and nonlinear equations) are displayed.</subfield>
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   <subfield code="a">Metadata rights reserved</subfield>
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