Doping topological Dirac semimetal with magnetic impurities: Electronic structure of Mn-doped <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Cd</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>As</mml:mi><m

The prospect of transforming a Dirac topological semimetal (TSM) into a Weyl TSM phase, following doping by magnetic impurities, is central to TSM applications. The magnetic field from polarized <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>d</a:mi></a:math> levels of magnetic impurities produces a field with a sharp local structure. To what extent magnetic impurities act in the same manner as an applied field and what are the effects of such a field on the electronic structure of a Dirac TSM are the subject of this paper. We present electronic structure calculations of bulk <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mrow><b:msub><b:mi>Cd</b:mi><b:mn>3</b:mn></b:msub><b:msub><b:mi>As</b:mi><b:mn>2</b:mn></b:msub></b:mrow></b:math> with substitutional doping of Mn impurities in the dilute alloy range. Quasiparticle <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mi>G</c:mi><c:mi>W</c:mi></c:mrow></c:math> (<d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mrow><d:mi>QS</d:mi><d:mi>G</d:mi><d:mi>W</d:mi></d:mrow></d:math>) electronic structure calculations are used in conjunction with <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mrow><e:mi>k</e:mi><e:mo>·</e:mo><e:mi>p</e:mi></e:mrow></e:math> model Hamiltonian calculations. As expected, we observe the splitting of the Dirac points into pairs of Weyl points following the doping with Mn. We also show that the electronic structure of Mn-doped <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:mrow><f:msub><f:mi>Cd</f:mi><f:mn>3</f:mn></f:msub><f:msub><f:mi>As</f:mi><f:mn>2</f:mn></f:msub></f:mrow></f:math> can be emulated by the electronic structure of pristine <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:msub><g:mi>Cd</g:mi><g:mn>3</g:mn></g:msub><g:msub><g:mi>As</g:mi><g:mn>2</g:mn></g:msub></g:mrow></g:math> with an appropriate external magnetic field. Some properties of the conductivity of bulk <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msub><h:mi>Cd</h:mi><h:mn>3</h:mn></h:msub><h:msub><h:mi>As</h:mi><h:mn>2</h:mn></h:msub></h:mrow></h:math> for different magnetic field orientations are also investigated. Our results inform future opportunities for unique device functionality based on band structure tuning not found in conventional magnetic Weyl TSM.