Developing approaches to effectively induce and control the magnetic states is critical to the use of magnetic nanostructures in quantum information devices but is still challenging. Here we have demonstrated, by employing the density functional theory calculations, the existence of infinite magnetic sheets with structural integrity and magnetic homogeneity. Examination of a series of transition metal dichalcogenides shows that the biaxial tensile strained NbS(2) and NbSe(2) structures can be magnetized with a ferromagnetic character due to the competitive effects of through-bond interaction and through-space interaction. The estimated Curie temperatures (387 and 542 K under the 10% strain for NbS(2) and NbSe(2) structures, respectively) suggest that the unique ferromagnetic character can be achieved above room temperature. The self-exchange of population between 4d orbitals of the Nb atom that leads to exchange splitting is the mechanism behind the transition of the spin moment. The induced magnetic moments can be significantly enhanced by the tensile strain, even giving rise to a half-metallic character with a strong spin polarization around the Fermi level. Given the recent progress in achieving the desired strain on two-dimensional nanostructures, such as graphene and a BN layer, in a controlled way, we believe that our calculated results are suitable for experimental verification and implementation, opening a new path to explore the spintronics in pristine two-dimensional nanostructures.
Voltage and capacity fading of layer structured lithium and manganese rich (LMR) transition metal oxide is directly related to the structural and composition evolution of the material during the cycling of the battery. However, understanding such evolution at atomic level remains elusive. On the basis of atomic level structural imaging, elemental mapping of the pristine and cycled samples, and density functional theory calculations, it is found that accompanying the hoping of Li ions is the simultaneous migration of Ni ions toward the surface from the bulk lattice, leading to the gradual depletion of Ni in the bulk lattice and thickening of a Ni enriched surface reconstruction layer (SRL). Furthermore, Ni and Mn also exhibit concentration partitions within the thin layer of SRL in the cycled samples where Ni is almost depleted at the very surface of the SRL, indicating the preferential dissolution of Ni ions in the electrolyte. Accompanying the elemental composition evolution, significant structural evolution is also observed and identified as a sequential phase transition of C2/m → I41 → Spinel. For the first time, it is found that the surface facet terminated with pure cation/anion is more stable than that with a mixture of cation and anion. These findings firmly established how the elemental species in the lattice of LMR cathode transfer from the bulk lattice to surface layer and further into the electrolyte, clarifying the long-standing confusion and debate on the structure and chemistry of the surface layer and their correlation with the voltage fading and capacity decaying of LMR cathode. Therefore, this work provides critical insights for design of cathode materials with both high capacity and voltage stability during cycling.
The isometric pyrochlore structure, A 2 B 2 O 7 , is generally susceptible to radiation damage, but certain compositions are remarkably resistant to radiation damage. In the binary system Gd 2 (Ti 2Ϫx Zr x )O 7 , the radiation resistance increases dramatically with the substitution of Zr for Ti, until the pure end member Gd 2 Zr 2 O 7 cannot be amorphized, even at doses as high as ϳ100 dpa. Although zirconate pyrochlores are generally considered to be radiation resistant, we report results for the amorphization of a zirconate pyrochlore La 2 Zr 2 O 7 by ion beam irradiation ͑ϳ5.5 dpa at room temperature͒. The critical amorphization temperature T c is low, ϳ310 K. The susceptibility to ion-beam-induced amorphization and structural disordering for zirconate pyrochlores is related to the structural deviation from the ideal fluorite structure, as reflected by the x parameter of the O 48f .
Capacity
and voltage fading of Li2MnO3 is a major challenge
for the application of this category of material, which is believed
to be associated with the structural and chemical evolution of the
materials. This paper reports the detailed structural and chemical
evolutions of Li2MnO3 cathode captured by using
aberration corrected scanning/transmission electron microscopy (S/TEM)
after certain numbers of charge–discharge cycling of the batteries.
It is found that structural degradation occurs from the very first
cycle and is spatially initiated from the surface of the particle
and propagates toward the inner bulk as the cyclic number increases,
featuring the formation of the surface phase transformation layer
and gradual thickening of this layer. The structure degradation is
found to follow a sequential phase transformation: monoclinic C2/m → tetragonal I41 → cubic spinel, which is consistently supported
by the decreasing lattice formation energy based on DFT calculations.
For the first time, high spatial resolution quantitative chemical
analysis reveals that 20% oxygen in the surface phase transformation
layer is removed and such a newly developed surface layer is a Li-depleted
layer with reduced Mn cations. This work demonstrates a direct correlation
between structural degradation and the cell’s electrochemical
degradation, which enhances our understanding of Li–Mn-rich
(LMR) cathode materials.
Developing efficient electrocatalysts for an oxygen evolution reaction (OER) is important for renewable energy storage. Here, we design high-density Ir single-atom catalysts supported by CoO x amorphous nanosheets (ANSs) for the OER. Experimental results show that Ir single atoms are anchored by abundant surface-absorbed O in CoO x ANSs. Ir single-atom catalysts possess ultrahigh mass activity that is 160-fold of commercial IrO 2 . The OER of IrCoO x ANSs reached a record low onset overpotential of less than 30 mV. In situ X-ray absorption spectroscopy reveals that Ir−O−Co pairs directly boosted the OER efficiency and enhanced the Ir stability.
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