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Non-trivial evolution of the Dirac cone in chromium doped Dirac semimetal Cd3As2
The magnetic doping of Dirac semimetals breaks their time-reversal symmetry thus giving rise to anomalous
transport phenomena promising for applications. While the Dirac cone (DC) manifestations were observed in the
electron transport of (Cd1 xCrx)3As2 alloys up to x = 0.06, their mechanism remains challenging. To address this
challenge, we performed DFT calculations of the (Cd0.96Cr0.04)3As2 alloy with the non-magnetic (NM), ferromagnetic (FM), and antiferromagnetic (AFM) spin orders. It was found that the NM state is unstable, while the
FM state has the lowest energy. The band structure analysis revealed that Cr 3d states are distributed in energy
not uniformly, but with Cr-free windows, in which the Dirac spectrum can survive. The only exception is the
Dirac point vicinity, where a narrow gap is formed. Outside the window, the DC band strongly hybridizes with
the Cr 3d states and disappears. Near EF, such a Cr-free window with the DC band exists only in the FM↓ state and
is absent in the NM, FM↑, and AFM states. The Fermi surface of FM (Cd1 xCrx)3As2 has two parts: the DC↓ sheet
with the velocity vF ≈ 1•106 m/s and several sheets with low vF, originating from Cr 3d↑ states. As an example of
transport properties, the dc conductivity of FM (Cd1 xCrx)3As2 was estimated. We found that at T→0 K the DC↓
electrons have a very large transport lifetime and therefore dominate in the conductivity. In this dominance, the
role of the Cr-free window is double: it ensures the DC↓ surviving and greatly reduces an admixture of Cr 3d↓
orbitals to DC↓ states, so suppressing the scattering of DC↓ electrons by doped Cr atoms. This mechanism looks
rather general and may be applied to the design of magnetic topological alloys.