Time-dependent Schwinger boson mean-field theory enables Néel vector switching in the honeycomb lattice antiferromagnet, with threshold fields that vary with lattice coordination number.
05 ·hthr s for 0 < t < t 1 t1: first minimum of m(t) b) 0.8 0.82 0.84 0.86 0.88 0.9 0.92 0.94 0.96 0.98 χ Fig
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Control of the N\'eel vector in the quantum antiferromagnetic honeycomb lattice
Time-dependent Schwinger boson mean-field theory enables Néel vector switching in the honeycomb lattice antiferromagnet, with threshold fields that vary with lattice coordination number.