[Paper Review] Anisotropic Dirac fermions in a Bi square net of SrMnBi2
This study identifies highly anisotropic Dirac fermions in the Bi square net of SrMnBi2 through first-principles calculations, angle-resolved photoemission spectroscopy (ARPES), and quantum oscillation measurements on high-quality single crystals. The Dirac cone exhibits a Fermi velocity anisotropy ratio of ~8, distinguishing it from isotropic Dirac fermions in graphene or topological insulators, and establishes the Bi square net as a new platform for anisotropic Dirac fermions with tunable electronic properties.
We report the highly anisotropic Dirac fermions in a Bi square net of SrMnBi2, based on a first principle calculation, angle resolved photoemission spectroscopy, and quantum oscillations for high-quality single crystals. We found that the Dirac dispersion is generally induced in the (SrBi)+ layer containing a double-sized Bi square net. In contrast to the commonly observed isotropic Dirac cone, the Dirac cone in SrMnBi2 is highly anisotropic with a large momentum-dependent disparity of Fermi velocities of ~ 8. These findings demonstrate that a Bi square net, a common building block of various layered pnictides, provide a new platform that hosts highly anisotropic Dirac fermions.
Motivation & Objective
- To identify and characterize Dirac fermions in the layered pnictide SrMnBi2, particularly within its Bi square net structure.
- To investigate whether the Bi square net—a common building block in layered pnictides—can host Dirac fermions with anisotropic dispersion.
- To determine the electronic structure and Fermi velocity anisotropy of Dirac fermions in SrMnBi2 using multiple experimental and theoretical techniques.
- To explore the potential of SrMnBi2 and related compounds as tunable platforms for anisotropic Dirac fermions with coupled magnetic or superconducting orders.
Proposed method
- First-principles calculations using the full-potential linearized augmented plane wave (FP-LAPW) method within the generalized gradient approximation (GGA) to model the electronic band structure.
- Angle-resolved photoemission spectroscopy (ARPES) with 24 eV photons at UVSOR beamline 7U, performed on cleaved single crystals under ultra-high vacuum (<7×10⁻¹¹ Torr).
- Quantum oscillation measurements using 6-probe magnetotransport in high magnetic fields up to 63 T at the Dresden High Magnetic Field Laboratory and up to 33 T at NHMFL.
- Analysis of Shubnikov–de Haas (SdH) oscillations to extract Fermi surface cross-sectional area, effective mass, scattering time, and Berry’s phase.
- Use of the Onsager relation (F = (Φ₀/2π²)Aₖ) to determine the Fermi surface cross-sectional area from the quantum oscillation frequency.
- SdH fan diagram analysis to extract the Berry’s phase from the intercept of 1/Bₙ vs. Landau level index n, with a non-zero intercept indicating Dirac fermions.
Experimental results
Research questions
- RQ1Does the Bi square net in SrMnBi2 host Dirac fermions with anisotropic dispersion, and if so, what is the degree of anisotropy in the Fermi velocity?
- RQ2What experimental evidence confirms the presence of Dirac fermions in SrMnBi2, particularly in terms of non-zero Berry’s phase and quantum oscillations?
- RQ3How does the electronic structure of SrMnBi2 differ from isotropic Dirac materials like graphene, particularly in terms of band dispersion and Fermi velocity anisotropy?
- RQ4Can the anisotropic Dirac cone in SrMnBi2 be tuned via chemical substitution of alkaline earth metals or pnictogens, and how does magnetic ordering in MnBi layers affect the Dirac state?
- RQ5What is the role of the (SrBi)+ layer and double-sized Bi square net in stabilizing the anisotropic Dirac cone?
Key findings
- The Dirac cone in SrMnBi2 exhibits a large momentum-dependent anisotropy in Fermi velocity, with a ratio of maximum to minimum v_F ≈ 8, indicating highly anisotropic Dirac fermions.
- ARPES measurements confirm a linear energy dispersion in the Bi square net, with a Dirac point located at the Γ point of the Brillouin zone.
- Quantum oscillation measurements reveal a single Fermi surface pocket with a frequency F = 152(5) T, corresponding to a cross-sectional area Aₖ = 1.45(5) nm⁻², or ~0.7% of the Brillouin zone.
- The cyclotron effective mass is measured as m_c = 0.29(2)mₑ, and the scattering time is τ = 3.5(5)×10⁻¹⁴ s⁻¹, yielding a mobility of ~250 cm²/Vs.
- The SdH fan diagram shows a non-zero intercept at n = -0.40(9), yielding a Berry’s phase of 0.5, confirming the presence of Dirac fermions with a non-trivial topological character.
- The combination of low effective mass, high mobility, and non-zero Berry’s phase establishes SrMnBi2 as a bulk Dirac material with anisotropic Dirac fermions hosted in the Bi square net.
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This review was created by AI and reviewed by human editors.