Ask a Question

Prefer a chat interface with context about you and your work?

Magnetism in Geometrically Frustrated<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>YMnO</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:math>under Hydrostatic Pressure Studied with Muon Spin Relaxation

Magnetism in Geometrically Frustrated<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>YMnO</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:math>under Hydrostatic Pressure Studied with Muon Spin Relaxation

The ferroelectromagnet ${\mathrm{YMnO}}_{3}$ consists of weakly coupled triangular layers of $S=2$ spins. Below ${T}_{N}\ensuremath{\approx}70\text{ }\text{ }\mathrm{K}$ muon-spin relaxation data show two oscillatory relaxing signals due to magnetic order, with no purely relaxing signals resolvable (which would require different coexisting spin distributions). The transition temperature ${T}_{N}$ increases with applied hydrostatic pressure, …