
arXiv: 2204.12795
At filling factor $ν=0,\pm1$, the ground state of graphene is a particular SU(4) ferromagnet which hosts a rich phase diagram along with several spin, pseudospin or "entanglement" magnon modes. Motivated by recent experiments, we study a $ν=-1|0|-1$ Fabry-Pérot magnonic junction. If the ground state at $ν=0$ is spin polarized, there exist two spin modes which interfere and create a beating pattern, while pseudospin modes are reflected. The same scenario occurs for pseudospin magnon if the $ν=0$ ground state is pseudospin polarized. The observation of such an interference pattern would provide information on the low-energy anisotropies and thus on the ground state.
6 pages, 3 figures
Spin polarization, Condensed Matter - Mesoscale and Nanoscale Physics, Graphenes, Filling factor, Spin-polarized, Rich phase, Fabry-Perot interferometers, FOS: Physical sciences, Physik (inkl. Astronomie), Spin dynamics, Quantum Hall ferromagnets, [PHYS] Physics [physics], Quantum entanglement, Scattering junction, Interference patterns, Mesoscale and Nanoscale Physics (cond-mat.mes-hall), Ferromagnetism, Fabry Perot interference, Pseudospin, Ferromagnets
Spin polarization, Condensed Matter - Mesoscale and Nanoscale Physics, Graphenes, Filling factor, Spin-polarized, Rich phase, Fabry-Perot interferometers, FOS: Physical sciences, Physik (inkl. Astronomie), Spin dynamics, Quantum Hall ferromagnets, [PHYS] Physics [physics], Quantum entanglement, Scattering junction, Interference patterns, Mesoscale and Nanoscale Physics (cond-mat.mes-hall), Ferromagnetism, Fabry Perot interference, Pseudospin, Ferromagnets
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