2015
DOI: 10.1039/c4cp05912c
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Reexamination of the origin of the pseudo Jahn–Teller puckering instability in silicene

Abstract: Silicene, the graphene-like crystal formed by the Si hexagonal lattice, presents a periodic buckled structure whose origin is due to the pseudo Jahn-Teller instability on each of its planar six membered rings. This has been attributed to the coupling of the planar D6h ground state with the first b2g excited state through a b2g vibrational mode. Here we show, by explicitly calculating the vibronic coupling constants through a complete study of the PJT effect, that the vibronic coupling of the ground state with … Show more

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Cited by 30 publications
(21 citation statements)
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“…The average bond lengths obtained with the methods B3LYP/TZ2P and TPSSH/TZ2P have very similar values with a maximum difference of 0.007 Å for D 2h and 0.019 Å for the distorted C 2h . It should be notice that the calculated bond lengths for the planar structure differ at most 0.043 Å compared to Si 6 H 6 (2.208 Å) [25], whose value is within the range of decasilanaphthalene. The Si 10 H 8 average puckering angle was of 36.6 for TPSSH/TZ2P and 40.5 for B3LYP/TZ2P; while a puckering angle of 30.9 and 40.0 were obtained for Si 6 H 6 with the same methods, respectively.…”
Section: Methodsmentioning
confidence: 95%
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“…The average bond lengths obtained with the methods B3LYP/TZ2P and TPSSH/TZ2P have very similar values with a maximum difference of 0.007 Å for D 2h and 0.019 Å for the distorted C 2h . It should be notice that the calculated bond lengths for the planar structure differ at most 0.043 Å compared to Si 6 H 6 (2.208 Å) [25], whose value is within the range of decasilanaphthalene. The Si 10 H 8 average puckering angle was of 36.6 for TPSSH/TZ2P and 40.5 for B3LYP/TZ2P; while a puckering angle of 30.9 and 40.0 were obtained for Si 6 H 6 with the same methods, respectively.…”
Section: Methodsmentioning
confidence: 95%
“…Jose and Datta [28] reported an average puckering angle of 33.7 and 34.3 for Si 6 H 6 and Si 10 H 8 , respectively, obtained with the methods M05-2X/TZVP and B3PW91/TZVP, which are closer to our TPSSH/TZ2P results. The HOMO-LUMO gaps obtained for planar Si 10 H 8 are 2.0 and 2.35 eV for TPSSH/TZ2P and B3LYP/TZ2P, respectively, against 3.31 and 2.94 eV for Si 6 H 6 with the same methods [25].…”
Section: Methodsmentioning
confidence: 96%
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“…13,14 Through folding of rings in heterocyclic compounds, symmetry breaking phenomenon has been reported in many studies and the instability of the ground state in planar configuration of those molecules and their coupling with excited states have been explained via PJTE theorem. [15][16][17][18][19][20][21][22][23][24][25][26][27] Restoring planarity in the systems that are puckered from their planar configurations due to the symmetry breaking phenomenon has been investigated through the PJTE. To do so, their planar configuration restores ether by coordinating two anions, cations, or rings up and down to the nonplanar systems [28][29][30] or influences the parameters of the PJTE instability by removing or adding electrons; 31 they show that symmetry breaking phenomenon is suppressed in the folded systems.…”
Section: Introductionmentioning
confidence: 99%