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·The spin orientation in synthetic hematite ilmenite samples and in a sample of natural hematite was studied from room temperature to above the antiferromagnetic paramagnetic phase transition the Nel temperature; T N ≈ 600 950 K by neutron powder diffraction and at room temperature by Mössbauer spectroscopy The usually assumed magnetic structure of
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·Structure of hematite 2 ×2 × 1 supercell spin density left with a single AFM plane highlighted in black shown color coded by distance from a central iron atom 0 middle
·We report on spin wave spectroscopy studies performed on the natural mineral hematite $alphatext{ Fe} 2text{O} 3$ which is a canted antiferromagnet By means of broadband GHz spectroscopy and inelastic light scattering we determine a damping coefficient of $times10^{ 5}$ and magnon group velocities of a few 10 km/s respectively at
·Spin wa ve dispersion of ultra low damping hematite α F e 2 O 3 at GHz frequencies Mohammad Hamdi 1 ∗ Ferdinand Posv a 1 and Dirk Grundler 1 2 † 1 ´
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·1 Introduction Hematite α Fe 2 O 3 is the most stable and widespread iron oxide mineral in has a corundum crystal structure with alternating iron and oxygen layers stacked along the crystallographic c axis of the hexagonal unit low temperatures Fe 3 spins order antiferromagnetically Shull et al 1951 so that moments in
·THz signals from the α Fe 2 O 3 /HM structures a Schematic of the transmission type THz spectroscopy setup The coordinate xyz is adapted to the laboratory sample is placed in the x y plane and the laser is incident along the magnetic field B ext is applied along y as shown in panel a or x not shown The
·We have synthesized 40 nm sized hematite particles by the forced hydrolysis of acid Fe<sup>3 </sup> solution to investigate the change in spin direction during the Morin transition
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·The total THz spin current dynamics can be manipulated by a medium‐strength magnetic field below 1 T The control of the THz spin current achieved in α‐Fe2O3 opens the pathway toward tailoring the exact spin current dynamics from ultrafast AFM spin sources Hematite α‐Fe2O3 is a promising model material in this respect because its
·Low magnetic damping and high group velocity of spin waves SWs or magnons are two crucial parameters for functional magnonic devices Magnonics research on signal processing and wave based computation at GHz frequencies focused on the artificial ferrimagnetic garnet Y 3 Fe 5 O 12 YIG so far We report on spin wave spectroscopy studies
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The spin flop transition of acicular hematite nanoparticles of different size synthesized by chemical route and annealed at different temperatures has been investigated as a function of
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·Figure 2 a Geometry used to investigate the nonlocal spin Seebeck effect NL SSE in hematite blue A passing charge current heats the hematite below one Pt wire generating a thermal gradient ∇ easy axis is inclined at 33 ∘ to the surface plane and a magnetic field H is applied parallel in the in plane component of the Nel vector b Local SSE
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·Monodisperse hematite α Fe2O3 nanoparticles were synthesized by forced hydrolysis of acidic Fe3 solution Rietveld analysis was applied to the X ray powder diffraction data to refine the
·Abstract Hematite α Fe2O3 is a potential photoanode material for photoelectrochemical PEC water splitting but its short hole diffusion length and low water oxidation kinetics prevent its practical application In general the hole transport rate and the water oxidation kinetics could be improved by modifying the oxygen evolution cocatalysts OECs in
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· Figure3 ManipulationofJs y byB AmplitudeofJ s y versusB ∥ yforlinearly red andcircularly blue polarizedpumppulsesand𝛽=120° Thesolid curvesaresigmoidfi TheadditionalcontributiontoJs y whileapplying B
·The hematite in Sinus Meridiani is thus distinct from the fine grained diameter <5 10 μm red crystalline hematite considered on the basis of visible near IR data to be a minor spectral
·Hematite chemically known as α Fe 2 O 3 First based on the orientation of the local spin density around the Fe atoms of α Fe 2 O 3 we found that the AFM 1 is the most energetically favorable magnetic configuration under all studied theories More interestingly we discovered that the expected outcomes vary significantly
·Hematite α Fe 2 O 3 is known to undergo conversion from weak ferromagnetic to antiferromagnetic as the temperature decreases below the Morin temperature T M = 250 K due to spin moment rotation occurring during the Morin transition MT = 250 K due to spin moment rotation occurring during the Morin transition MT
