Janus graphene nanoribbons with localized states on a single zigzag edge

Jun 8, 2024
19 pages
Published in:
  • Nature 637 (2025) 8046, 580-586
  • Published: Jan 8, 2025
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Abstract: (Springer)
Topological design of π electrons in zigzag-edged graphene nanoribbons (ZGNRs) leads to a wealth of magnetic quantum phenomena and exotic quantum phases1,2,3,4,5,6,7,8,910^{1, 2, 3, 4, 5, 6, 7, 8, 9–10}. Symmetric ZGNRs typically show antiferromagnetically coupled spin-ordered edge states1,2^{1,2}. Eliminating cross-edge magnetic coupling in ZGNRs not only enables the realization of a class of ferromagnetic quantum spin chains11^{11}, enabling the exploration of quantum spin physics and entanglement of multiple qubits in the one-dimensional limit3,12^{3,12}, but also establishes a long-sought-after carbon-based ferromagnetic transport channel, pivotal for ultimate scaling of GNR-based quantum electronics1,23,9,13^{1, 2–3,9,13}. Here we report a general approach for designing and fabricating such ferromagnetic GNRs in the form of Janus GNRs (JGNRs) with two distinct edge configurations. Guided by Lieb’s theorem and topological classification theory14,1516^{14, 15–16}, we devised two JGNRs by asymmetrically introducing a topological defect array of benzene motifs to one zigzag edge, while keeping the opposing zigzag edge unchanged. This breaks the structural symmetry and creates a sublattice imbalance within each unit cell, initiating a spin-symmetry breaking. Three Z-shaped precursors are designed to fabricate one parent ZGNR and two JGNRs with an optimal lattice spacing of the defect array for a complete quench of the magnetic edge states at the ‘defective’ edge. Characterization by scanning probe microscopy and spectroscopy and first-principles density functional theory confirms the successful fabrication of JGNRs with a ferromagnetic ground-state localized along the pristine zigzag edge.
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  • 19 pages, 4 figures