Grigor Adamyan’s scientific contributions

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Publications (3)


Helical edge modes in a triangular Heisenberg antiferromagnet
  • Article

December 2024

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3 Reads

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1 Citation

Physical Review B

Bastián Pradenas

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Grigor Adamyan

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Oleg Tchernyshyov

FIG. 3. An example of a conformal map w(z) (26) that transforms a straight boundary into a curved one with a bulge.
Conformal maps and edge mode attenuation on imperfect boundaries
  • Preprint
  • File available

December 2024

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23 Reads

We developed a conformal map technique to analyze the attenuation of edge modes propagating along imperfect boundaries. In systems where the potential energy exhibits conformal invariance, the conformal transformation can straighten the boundary, simplifying the boundary conditions. Using the example of edge modes in a simple field-theoretical model, we examined scattering into the bulk and identified conditions that ensure the robustness of edge modes against damping. This technique has the potential to be applied to other edge-mode problems in 2+1 dimensions.

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FIG. 1. (a) Magnetic order in a Heisenberg antiferromagnet on a triangular lattice. The shaded area is a magnetic unit cell. (b) The magnetic order parameter. (c) The corresponding spin-frame vectors.
FIG. 3. (a) Details of the superexchange model. Small red and blue triangles are non-magnetic ions of two different types mediate superexchange of strengths J △ = J(1 + ∆)/2 and J ▽ = J(1 − ∆)/2. (b) The resulting spin model has exchange interactions of strengths J in the bulk (black solid lines), J(1+ ∆)/2 on red dotted external edges, and J(1 − ∆)/2 on blue dashed external edges.
FIG. 4. Geometry of the triangular lattice. Red, gren, and blue dots mark sites of magnetic sublattices 1, 2, and 3, respectively. The shaded area is the magnetic unit cell centered on a site of sublattice 3.
Helical edge modes in a triangular Heisenberg antiferromagnet

August 2024

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39 Reads

We investigate the emergence of helical edge modes in a Heisenberg antiferromagnet on a triangular lattice, driven by a topological mechanism similar to that proposed by Dong et al. [Phys. Rev. Lett. 130, 206701 (2023)] for chiral spin waves in ferromagnets. The spin-frame field theory of a three-sublattice antiferromagnet allows for a topological term in the energy that modifies the boundary conditions for certain polarizations of spin waves and gives rise to edge modes. These edge modes are helical: modes with left and right circular polarizations propagate in opposite directions along the boundary in a way reminiscent of the electron edge modes in two-dimensional topological insulators. The field-theoretic arguments are verified in a realistic lattice model of a Heisenberg antiferromagnet with superexchange interactions that exhibits helical edge modes. The strength of the topological term is proportional to the disparity between two inequivalent superexchange paths. These findings suggest potential avenues for realizing magnonic edge states in frustrated antiferromagnets without requiring Dzyaloshinskii-Moriya interactions or nontrivial magnon band topology.

Citations (1)


... The parameters ρ = χS 2 and µ describe the inertial and exchange stiffness properties of the antiferromagnet, respectively. The final term, which is topological in nature and weighted by λ, reduces to a boundary contribution in the bulk and is responsible for the emergence of localized helical edge modes [19]. In what follows, we ignore this term for the bulk analysis. ...

Reference:

Spontaneous symmetry breaking in the Heisenberg antiferromagnet on a triangular lattice
Helical edge modes in a triangular Heisenberg antiferromagnet
  • Citing Article
  • December 2024

Physical Review B