We present a theoretical study of structural evolution,
electronic
properties, and photoelectron spectra of two sulfur atom-doped boron
clusters S2B
n
0/– (n = 2–13), which reveal that the global
minima of the S2B
n
0/– (n = 2–13) clusters show an evolution from
a linear-chain structure to a planar or quasi-planar structure. Some
S-doped boron clusters have the skeleton of corresponding pure boron
clusters; however, the addition of two sulfur atoms modified and improved
some of the pure boron cluster structures. Boron is electron-deficient
and boron clusters do not form linear chains. Here, two sulfur atom
doping can adjust the pure boron clusters to a linear-chain structure
(S2B2
0/–, S2B3
0/–, and S2B4
–), a quasi-linear-chain structure (S2B6
–), single- and double-chain structures
(S2B6 and S2B9
–), and double-chain structures (S2B5, and S2B9). In particular, the smallest linear-chain boron
clusters S2B2
0/– are shown
with an S atom attached to each end of B2. The S2B2 cluster possesses the largest highest occupied molecular
orbital (HOMO)–lowest unoccupied molecular orbital (LUMO) gap
of 5.57 eV and the S2B2
– cluster
possesses the largest average binding energy E
b of 5.63 eV, which shows the superior chemical stability and
relative stability, respectively. Interestingly, two S-atom doping
can adjust the quasi-planar pure boron clusters (B7
–, B10
–, and B12
0/–) to a perfect planar structure. AdNDP bonding
analyses reveal that linear S2B3 and planar
SeB11
– have π aromaticity and σ
antiaromaticity; however, S2B2, planar S2B6, and planar S2B7
– clusters have π antiaromaticity and σ aromaticity. Furthermore,
AdNDP bonding analyses reveal that planar S2B4, S2B10, and S2B12 clusters
are doubly (π and σ) aromatic, whereas S2B5
–, S2B8, S2B9
–, and S2B13
– clusters are doubly (π and σ) antiaromatic.
The electron localization function (ELF) analysis shows that S2B
n
0/– (n = 2–13) clusters have different electron delocalization
characteristics, and the spin density analysis shows that the open-shell
clusters have different characteristics of electron spin distribution.
The calculated photoelectron spectra indicate that S2B
n
– (n = 2–13)
have different characteristic peaks that can be compared with future
experimental values and provide a theoretical basis for the identification
and confirmation of these doped boron clusters. Our work enriches
the new database of geometrical structures of doped boron clusters,
provides new examples of aromaticity for doped boron clusters, and
is promising to offer new ideas for nanomaterials and nanodevices.