Abstract:Structural transition from inverse sandwich Ta2B7+ (1) and Ta2B8 (2) with σ + π dual aromaticity to the smallest metallo-borospherene D3h Ta3B12− (3) which is σ + π + δ triply aromatic in nature.
“…We also reported the smallest metallo-borospherene D 3h Ta 3 B 12 − composed of two eclipsed B 3 triangles on the top and bottom interconnected by three B 2 units on the waist [27]. However, to the best of our knowledge, there have been no experimental or theoretical evidence reported on tetra-La-doped boron clusters to date.…”
Cage-like and core-shell metallo-borospherenes exhibit interesting structures and bonding. Based on extensive global searches and rst-principles theory calculations, we predict herein the perfect tetrahedral cage-like T d La 4 B 24 (1) and core-shell T d La 4 B 29 (2), T d La 4 B 29 + (3), and T d La 4 B 29 -(4) which all possess the same geometrical symmetry as their carbon fullerene counterpart T d C 28 , with four equivalent interconnected B 6 triangles on the cage surface and four nona-coordinate La centers in four conjoined η 9 -B 9 rings. In these tetra-La-doped boron complexes, La 4 [B@B 4 @B 24 ] 0/+/-(2/3/4) in the structural motif of1+4+28 contain a B-centered tetrahedral T d B@B 4 core in a La-decorated tetrahedral La 4 B 24 shell, with the negatively charged tetra-coordinate Bat the center being the boron analog of tetrahedral C in T d CH 4 (B -C). Detailed orbital and bonding analyses indicate that these T d lanthanide boride complexes are spherically aromatic in nature with a universal La--B 9 (d-p) σ and (d-p) δ coordination bonding pattern.The IR, Raman, and UV-Vis or photoelectron spectra of these novel metallo-borospherenes are computationally simulated to facilitate their spectral characterizations.
“…We also reported the smallest metallo-borospherene D 3h Ta 3 B 12 − composed of two eclipsed B 3 triangles on the top and bottom interconnected by three B 2 units on the waist [27]. However, to the best of our knowledge, there have been no experimental or theoretical evidence reported on tetra-La-doped boron clusters to date.…”
Cage-like and core-shell metallo-borospherenes exhibit interesting structures and bonding. Based on extensive global searches and rst-principles theory calculations, we predict herein the perfect tetrahedral cage-like T d La 4 B 24 (1) and core-shell T d La 4 B 29 (2), T d La 4 B 29 + (3), and T d La 4 B 29 -(4) which all possess the same geometrical symmetry as their carbon fullerene counterpart T d C 28 , with four equivalent interconnected B 6 triangles on the cage surface and four nona-coordinate La centers in four conjoined η 9 -B 9 rings. In these tetra-La-doped boron complexes, La 4 [B@B 4 @B 24 ] 0/+/-(2/3/4) in the structural motif of1+4+28 contain a B-centered tetrahedral T d B@B 4 core in a La-decorated tetrahedral La 4 B 24 shell, with the negatively charged tetra-coordinate Bat the center being the boron analog of tetrahedral C in T d CH 4 (B -C). Detailed orbital and bonding analyses indicate that these T d lanthanide boride complexes are spherically aromatic in nature with a universal La--B 9 (d-p) σ and (d-p) δ coordination bonding pattern.The IR, Raman, and UV-Vis or photoelectron spectra of these novel metallo-borospherenes are computationally simulated to facilitate their spectral characterizations.
“…The previous studies proved the feasibility of the PBE0 functional 45 to describe the energy differences between different isomers of TM doped B clusters. 35,37,39,[46][47][48] Moreover, our previous study of the single TM atom doped B n (n ¼ 7-10) clusters 49 also conrmed that PBE0 functional can precisely describe the interactions between TM atom and B atom by comparing with the high-level CCSD(T) 50 results. For basis set, the 6-311G* was proved enough to describe B atom in our study of pure boron clusters.…”
Section: Methodsmentioning
confidence: 99%
“…(i) planar molecular wheel, [21][22][23] (ii) half-sandwich, 24 inverse sandwich 25,26 and inverse triple-decker 27 clusters, (iii) drum-like structures, [28][29][30] (iv) the endohedral boron cages, [31][32][33][34] and (v) metallo-borospherenes. [35][36][37][38] Doping single TM atom into small-sized B clusters produces perfect TM-centered monocyclic B wheel clusters such as Co@B 8 À , 21 Rh@B 9 À , 22 and Ta@B 10 À . 23 The 10 coordination number (CN) of Ta@B 10 À is known as the highest number among the planar species.…”
Section: Introductionmentioning
confidence: 99%
“…units on the waist,37 the lowest energy structures of Hf 4 B 18 and Ta 4 B 18 possess a large E HL of 2.60 and 2.61 eV, respectively, being less chemically reactive than others. For all anionic clusters, due to the trapping of an electron, the E HL of these species is decreased and signicantly less than the neutral clusters.…”
“… 32 The smallest tri-Ta-doped spherical trihedral metallo-borospherene D 3h Ta 3 B 12 – ( 1 ) has been very recently predicted by our group, which consists of two eclipsed B 3 triangles on the top and bottom interconnected by three B 2 units on the waist. 33 However, there have been no experimental or theoretical evidence reported on tetra-Ta-doped boron clusters to date. Tetra-metal-doped endohedral metallo-silicon fullerenes T d M 4 Si 28 (M = Al and Ga) have been theoretically proposed to possess the same tetrahedral symmetry as their fullerene counterpart T d C 28 .…”
Cage-like metallo-borospherenes
exhibit unique structures and bonding.
Inspired by the newly reported smallest spherical trihedral metallo-borospherene
D
3h
Ta
3
B
12
–
(
1
), which contains two equivalent B
3
triangles
interconnected by three B
2
units on the cage surface, we
present herein a first-principles theory prediction of the perfect
spherical tetrahedral metallo-borospherene
T
d
Ta
4
B
18
(
2
), which possesses
four equivalent B
3
triangles interconnected by six B atoms,
with four equivalent nonacoordinate Ta centers in four η
9
-B
9
rings as integrated parts of the cage surface.
As the well-defined global minimum of the neutral, Ta
4
B
18
(
2
) possesses four 10c-2e B
9
(π)–Ta(d
σ
) and eight 10c-2e B
9
(π)–Ta(d
δ
) coordination bonds evenly distributed over four Ta-centered
Ta@B
9
nonagons, with the remaining 18 valence electrons
in nine 22c-2e totally delocalized bonds following the 18-electron
principle (1S
2
1P
6
1D
10
) of a superatom.
Such a bonding pattern renders spherical aromaticity to the tetrahedral
complex, which can be used as building blocks to form the face-centered
cubic crystal Ta
4
B
15
(
3
). The IR,
Raman, and UV–vis spectra of Ta
4
B
18
(
2
) are theoretically simulated to facilitate its future experimental
characterizations.
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