IWCN 2021: A Practical Peierls Phase Recipe for Periodic Atomistic Systems Under Magnetic Fields

By Alessandro Cresti

Université Grenoble Alpes, University Savoie Mont Blanc, CNRS, Grenoble INP, IMEP-LAHC, Grenoble, France

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Abstract

The Peierls phase conveniently describes the orbital effect of a relatively weak magnetic field B on atomistic systems represented by a tight-binding-like Hamiltonian [1]. The phase multiplies the Hamiltonian elements between couples of atomic orbitals and is proportional to the line integral of the vector potential A (with B = × A) along the straight path between them. The Peierls phase changes under gauge transformations A → A + ∇χ, but its circulation as well as the physical observables are gauge independent.

For periodic systems, or systems with periodic components (as contacts and probes in a Hall bar), a generic gauge will not guarantee the Hamiltonian to be invariant under spatial translations. However, this invariance is desirable to allow the use of convenient techniques for electronic structure and transport simulations, as the Bloch theorem for the Hamiltonian diagonalization, or the Sancho-Rubio algorithm [2] for determining the contact self-energies.

In this contribution, by a proper gauge choice, I will provide general ready-to-use formulas to determine Peierls phase factors that preserve the translation symmetry of any periodic quasi-one-dimensional or two-dimensional system under a homogeneous magnetic field [3]. Some examples of applications will be briefly illustrated, see figures. First, I will present the case of a metallic carbon nanotube in high magnetic fields. Depending on the angle between field and nanotube axis, the electronic structure exhibits a rich physics ranging from Landau states to Aharonov-Bohm effect. Then, based on Green’s function transport simulations, we will discuss the importance of disorder for the observation of extended Hall resistance plateaus in 2DEG Hall bars. Finally, I will present the case of periodic 2D graphene with Gaussian bumps, where the induced strain makes Landau levels dispersive and lifts the valley degeneracy.

The provided formulas represent a practical and useful tool for the simulation of electronic and transport properties of mesoscopic systems in the presence of magnetic fields.

Figures

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References

  1. [1] R. Peierls, Z. Phys., 80, 763 (1933).
  2. M. P. Lopez Sancho et al., J. Phys. F, 15, 851 (1985).
  3. A. Cresti, Phys. Rev. B., 103, 045402 (2021).

Cite this work

Researchers should cite this work as follows:

  • Alessandro Cresti (2021), "IWCN 2021: A Practical Peierls Phase Recipe for Periodic Atomistic Systems Under Magnetic Fields," https://nanohub.org/resources/35266.

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IWCN 2021: A Practical Peierls Phase Recipe for Periodic Atomistic Systems Under Magnetic Fields
  • A practical Peierls phase recipe for periodic atomistic systems under magnetic fields   Alessandro Cresti   Univ. Grenoble Alpes, Univ. Savoie Mont Blanc, CNRS, Grenoble INP, IMEP-LAHC, 38000 Grenoble, France alessandro.cresti@grenoble-inp.fr 1. A practical Peierls phase reci… 0
    00:00/00:00
  • Plan of the presentation 2. Plan of the presentation 11.344678011344678
    00:00/00:00
  • Tight-binding-like Hamiltonian and Peierls phase 3. Tight-binding-like Hamiltonian… 37.470804137470807
    00:00/00:00
  • The problem of periodicity 4. The problem of periodicity 101.93526860193528
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  • Periodic 2D system 5. Periodic 2D system 134.1675008341675
    00:00/00:00
  • Periodic 2D system 6. Periodic 2D system 219.85318651985318
    00:00/00:00
  • Periodic 2D system 7. Periodic 2D system 262.72939606272939
    00:00/00:00
  • Periodic 2D system 8. Periodic 2D system 341.74174174174175
    00:00/00:00
  • Periodic 2D system 9. Periodic 2D system 399.13246579913249
    00:00/00:00
  • Periodic 2D system 10. Periodic 2D system 433.46680013346679
    00:00/00:00
  • Example of a quasi 1D system: a 2DEG Hall bar 11. Example of a quasi 1D system: … 458.72539205872539
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  • Conclusion 12. Conclusion 546.8134801468135
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