Effective
hydrogen (H2) production with surface engineering of less
active catalysts by an innovative approach is followed here. In this
work, a non-noble 2H phase of VS2 layers, which showed
poor activity for hydrogen evolution reaction (HER) in 0.5 M H2SO4, was made highly active by decorating palladium
(Pd) nanoparticles (NPs) over VS2 layers. A density functional
theory (DFT) study confirmed the successful binding of Pd with VS2, and the bond length in a Pd4 tetrahedron was
measured to be 2.60 Å. In VS2–Pd, Pd as a Pd4 tetrahedron is pointed toward the VS2 layer, and
the calculated Pd–S bond distance is 2.42 Å with some
expansion of three Pd–Pd bonds (2.85 Å). From the density
of states, it was confirmed that the band gap was too high for VS2 (0.2 eV; 2H phase) and was reduced to nearly zero in VS2–Pd (0.05 eV). In the electrocatalytic HER part, the
obtained ΔG
H values from DFT were
0.05, −0.45, and 0.22 eV for VS2/Pd4,
Pd4, and VS2, respectively, which imply that
VS2–Pd4 had improved HER activity compared
to pristine VS2 and Pd4. A concentration-dependent
study was carried out with molar ratios of Pd at 0.01, 0.05, and 0.1
M with VS2 layers. From the HER polarization study, VS2–Pd (0.05 M) showed an overpotential of 157 mV at 20
mA cm–2, which is 373 mV less than only VS2 with a Tafel slope of 75 mV dec–1 with overwhelming
stability. These highly promising results will be interesting to make
less active stable phases by incorporating metal NPs for efficient
and stable H2 production.
Herein,
we employed first-principles density functional theory
calculations to understand the structural, electronic, and magnetic
properties of pristine and lithiated zinc blende (ZB) SiC(111) surface
slabs. Our calculations on below four layer thick slabs reveal the
spontaneous formation of a graphitic SiC layer which mimics the two-dimensional
boron nitride structure. Though this monolayer shows a direct band
gap, the energy bands in bi- and trilayer slabs are nondegenerated
owing to weak van der Waal’s interaction between the layers,
and they show indirect band gap for those cases. In a pristine slab,
the surface states presented in both sides originate magnetism, and
they are coupled antiferromagnetically. Its strength decreases with
increasing layer thickness. This magnetism is quenched during lithiation
and exfoliation of layers. The latter is observed, even for thicker
ZB slabs during lithiation. The average lithium intercalation potential
is calculated to be 0.20 V, which is quite comparable with the anodic
potential of high capacity SiC nanoparticles as reported in experiment.
Thus, the mechanism of lithiation in SiC nanoparticles is proposed
to be intercalation, rather than alloying.
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