2020
DOI: 10.1016/j.scib.2019.11.003
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Ultrahigh-strain ferroelasticity in two-dimensional honeycomb monolayers: from covalent to metallic bonding

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Cited by 25 publications
(19 citation statements)
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“…In addition to the variation of the barrier height, we also analyzed the change of FE polarization and the Born effective charges (BECs) for the C 2 O 2 Fe monolayer at different strains. First, using the BEC method, 55 the FE polarization in the magnetic ground state was calculated mainly at 20%, 25% and 30% strain, as shown in Table 3. Although the intensity of FE polarization tends to decrease with increasing strains, it remains 1.609 × 10 −10 C m −1 at 30% strain.…”
Section: Resultsmentioning
confidence: 99%
“…In addition to the variation of the barrier height, we also analyzed the change of FE polarization and the Born effective charges (BECs) for the C 2 O 2 Fe monolayer at different strains. First, using the BEC method, 55 the FE polarization in the magnetic ground state was calculated mainly at 20%, 25% and 30% strain, as shown in Table 3. Although the intensity of FE polarization tends to decrease with increasing strains, it remains 1.609 × 10 −10 C m −1 at 30% strain.…”
Section: Resultsmentioning
confidence: 99%
“…Currently, based on the first-principles calculation, Lei et al provided an insight into the layered PdSe 2 material with ferroelastic phase transition (FPT) and also demonstrated that this phase transition can cause the transition of electronic structure from semiconductor to metal under uniaxial stress. , Therefore, we wonder whether there will be the thermal switching of layered PdSe 2 material in the process of FPT. Commonly, ferroelastic material, a phase change material, can convert from one stable phase to another equally stable phase under strain. It can realize switchable electronic, mechanical, thermal, and other properties. Here, we explore switchable κ L in ferroelastic PdSe 2 .…”
Section: Introductionmentioning
confidence: 99%
“…The state B has the same energy as state A but possesses a 120° lattice rotation, as highlighted by the colored ZrX chains in Figure . This is in a great contrast to conventional orthogonal swapping, as observed in TiN, α-ZrPI, , stanene, phosphorene, and phosphorene analogues . The spontaneous driving energies for this abnormal switching are 0.93 (39), 0.90 (38), and 0.57 eV (24 meV / atom) for the ZrCl 2 , ZrBr 2 , and ZrI 2 monolayers (Figure d), respectively.…”
mentioning
confidence: 78%