2021
DOI: 10.1088/1674-1056/ac2e63
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Molecular beam epitaxy growth of monolayer hexagonal MnTe2 on Si(111) substrate*

Abstract: Monolayer MnTe2 stabilized as 1T structure has been theoretically predicted to be a two-dimensional (2D) ferromagnetic metal and can be tuned via strain engineering. There is no naturally van der Waals (vdW) layered MnTe2 bulk, leaving mechanical exfoliation impossible to prepare monolayer MnTe2. Herein, by means of molecular beam epitaxy (MBE), we successfully prepared monolayer hexagonal MnTe2 on Si(111) under Te rich condition. Sharp reflection high-energy electron diffraction (RHEED) and low-energy electro… Show more

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Cited by 8 publications
(8 citation statements)
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“…Distinct from previously reported Mn chalcogenides of α-MnTe (rock-salt) 38 or MnSe 2 (MnTe 2 ) (pyrite), 39,40 our epitaxial Mn 2 Te 2 phase is stabilized in a DLHC structure with the lowest formation energy when thinned down, 41 similar to CuI or recently discovered Mn 2 Se 2 /NbSe 2 . 42 As shown in Figure 1a, the DLHC phase is in a layered structure with each quadruple layer separated by a vdW gap, within which a pair of buckled honeycomb Mn−Te double-layers are vertically bonded (simply named as MnTe).…”
contrasting
confidence: 83%
“…Distinct from previously reported Mn chalcogenides of α-MnTe (rock-salt) 38 or MnSe 2 (MnTe 2 ) (pyrite), 39,40 our epitaxial Mn 2 Te 2 phase is stabilized in a DLHC structure with the lowest formation energy when thinned down, 41 similar to CuI or recently discovered Mn 2 Se 2 /NbSe 2 . 42 As shown in Figure 1a, the DLHC phase is in a layered structure with each quadruple layer separated by a vdW gap, within which a pair of buckled honeycomb Mn−Te double-layers are vertically bonded (simply named as MnTe).…”
contrasting
confidence: 83%
“…Next, we explore the electronic and magnetic properties of the H@MnX monolayers. In pristine MnX monolayers, each Mn 2+ ion possesses a half-occupied d shell (d 5 ) and carries a large formal magnetic moment of 5 μ B . Because of the lack of itinerant carriers, the magnetic couplings in MnX are dominated by the superexchange interaction.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…Nevertheless, J 3 is AFM and is much larger in magnitude than J 1 and J 2 . Such a strong AFM coupling is due to two reasons: (i) One of the two Mn ions connected by J 3 has an occupation state of d 5 , which decides that J 3 must be AFM. (ii) The two Mn−X 4 tetrahedrons connected by J 3 are edgesharing.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
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