2019
DOI: 10.1038/s41565-019-0467-1
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Defect induced, layer-modulated magnetism in ultrathin metallic PtSe2

Abstract: Defects are ubiquitous in solids, often introducing new properties that are absent in pristine materials. One of the opportunities offered by these crystal imperfections is an extrinsically induced long-range magnetic ordering,1 a long-time subject of theoretical investigations.1-3 Intrinsic, two-dimensional (2D) magnetic materials4-7 are attracting increasing attention for their unique properties including layer-dependent magnetism4 and electric field modulation6. Yet, inducing magnetism into otherwise non-ma… Show more

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Cited by 201 publications
(184 citation statements)
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“…Whereas defect‐free PtSe 2 is diamagnetic, a transition to a half‐metallic ferromagnetic state for monolayer PtSe 2 at a critical strain of 5 % was predicted, which favors the formation of single Pt vacancies and may cause the p‐type conductance in PtSe 2. These point defects occur intrinsically in ultrathin 1 T ‐PtSe 2 layers, and Avsar et al . verified the emergence of magnetism as a result of vacancies in ultrathin metallic PtSe 2 both experimentally and theoretically.…”
Section: Properties and Applicationsmentioning
confidence: 89%
See 1 more Smart Citation
“…Whereas defect‐free PtSe 2 is diamagnetic, a transition to a half‐metallic ferromagnetic state for monolayer PtSe 2 at a critical strain of 5 % was predicted, which favors the formation of single Pt vacancies and may cause the p‐type conductance in PtSe 2. These point defects occur intrinsically in ultrathin 1 T ‐PtSe 2 layers, and Avsar et al . verified the emergence of magnetism as a result of vacancies in ultrathin metallic PtSe 2 both experimentally and theoretically.…”
Section: Properties and Applicationsmentioning
confidence: 89%
“…Bulk 1 T ‐PdTe 2 is metallic and diamagnetic and was predicted to undergo a transition to a narrow‐gap semiconductor (about 0.14 eV) as a monolayer, whereas our calculations suggest a semimetallic state when SOC is included (Figures S11 and S12). Weak, temperature‐independent paramagnetism (μ≪μ B ) is usually observed, which might be caused by defects . PdTe 2 features rather strong interlayer interactions, but with a cleavage energy of 0.85 J m −2 , it should still be exfoliable (Table ).…”
Section: Properties and Applicationsmentioning
confidence: 99%
“…In these systems, the pivotal role played by the single-ion anisotropies preserves magnetic order in low dimensions [16], as unambiguously demonstrated by the groundbreaking exfoliation of the bulk ferromagnet CrI 3 down to the monolayer limit [17], rapidly followed by the appearance of many other ultrathin magnets, e.g. Fe 3 GeTe 2 , Cr 2 Ge 2 Te 6 , FePSe 3 [14,15,[18][19][20] Within the constantly expanding family of twodimensional magnets, semiconducting thin films of CrI 3 are arguably the most prototypical members. They exhibit a layered crystal structure, in which Cr atoms are located at the corners of in-plane honeycomb networks and reside in edge-sharing octahedra formed by I atoms [21].…”
mentioning
confidence: 99%
“…Während defektfreies PtSe 2 diamagnetisch ist, wurde ein Übergang zu einem halbmetallischen ferromagnetischen Zustand bei Monolagen von PtSe 2 unter einer kritischen Streckung von 5 % vorhergesagt, was die Bildung von einzelnen Pt‐Fehlstellen fördert und der Grund für die p‐Typ‐Leitung in PtSe 2 sein könnte. Diese Punktdefekte tauchen intrinsisch in ultradünnen Schichten von 1 T ‐PtSe 2 auf, und Avsar et al . haben den daraus resultierenden Magnetismus experimentell und theoretisch bestätigt.…”
Section: Eigenschaften Und Anwendungenunclassified