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Publisher's Note: Interplay of magnetism and superconductivity in the compressed Fe-ladder compound BaFe 2 Se 3 [Phys. Rev. B 95 , 241109(R) (2017)]
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Magnetic and structural properties of the iron oxychalcogenides La 2 O 2 Fe 2 O M 2 ( M = S , Se )
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Spectroscopy and lifetime measurements in Ge 66 , Se 69 , and Ga 65 using fragmentation reactions
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Unraveling Photoinduced Spin Dynamics in the Topological Insulator Bi 2 Se 3
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Superconducting Phase Induced by a Local Structure Transition in Amorphous Sb[subscript 2]Se[subscri
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Structural evolution and skyrmionic phase diagram of the lacunar spinel GaMo[subscript 4]Se[subscript 8]
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Preferential hole defect formation in monolayer W Se 2 by electron-beam irradiation
Monolayer transition-metal dichalcogenides (TMDCs) have been extensively studied due to their wide range of physical properties and applications. It has been demonstrated that the electron beam in a transmission electron microscope (TEM) or scanning TEM (STEM) generates chalcogen vacancies that agglomerate into dispersed linelike or holelike defects. Here we employ a STEM electron beam and demonstrate that, in WSe 2 , beam-induced chalcogen vacancies initially form certain dispersed multivacancy structures, as seen in TMDCs in prior work. However, with suitable control of the STEM focused electron beam, these multivacancies gradually evolve into a dense network of ten-, 12-, 14-, and 16-member ring round holes, whereas the same process leads predominantly to chalcogen-vacancy line defects in other trigonal-prismatic TMDCs. Density functional theory calculations find that the underlying atomic-scale processes lead preferentially to defect structures that lower the total energy so that we are able to track the formation of the observed multivacancy complexes, which then lead to the formation of dense large round holes in WSe 2 . The same processes in WS 2 , however, are energetically unfavorable, while linear multivacancy defects are preferred, as observed. The demonstrated control of the formation of unique high-density round holes in WSe 2 has potential for applications such as atomic and molecular sieving.
Suppression of axionic charge density wave and onset of superconductivity in the chiral Weyl semimetal Ta 2 Se 8 I
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La 2 O 3 Mn 2 Se 2 : A correlated insulating layered d-wave altermagnet
Altermagnets represent a new class of magnetic phases without net magnetization, invariant under a combination of rotation and time reversal. Unlike conventional collinear antiferromagnets (AFM), altermagnets could lead to new correlated states and important material properties deriving from their nonrelativistic spin-split band structure. Indeed, they serve as the magnetic analogue of unconventional superconductors and can yield spin-polarized electrical currents in the absence of external magnetic fields, making them promising candidates for next-generation spintronics. Here, we report altermagnetism in the correlated insulator, magnetically ordered tetragonal oxychalcogenide, La 2 O 3 Mn 2 Se 2 . Symmetry analysis reveals a 𝑑 𝑥 2 −𝑦 2 -wave-like spin-momentum locking arising from the Mn 2 O Lieb lattice, supported by density functional theory (DFT) calculations. Magnetic measurements confirm the AFM transition below ∼166K while neutron pair distribution function analysis reveals a 2D short-range magnetic order that persists above the Néel temperature. Single crystals are grown and characterized using x-ray diffraction, optical and electron microscopy, and micro-Raman spectroscopy to confirm the crystal structure, stoichiometry, and uniformity. Furthermore, our findings establish La 2 O 3 Mn 2 Se 2 as a model altermagnetic system realized on a Lieb lattice.
Surface charge induced Dirac band splitting in a charge density wave material ( Ta Se 4 ) 2 I
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