The DFT calculations indicated dual-SPO intermediate
B is a trigonal bipyramidal structure with the apical Al coordination (
Fig. 5a). There is a non-negligible Ni-Al covalent interaction in
B, which can be demonstrated from the electron localization function (ELF). The frontier orbital (HOMO-1) of Ni's
dz2 electrons donated to 3p vacant orbitals of Al, suggesting the Ni(0) can be stabilized by Lewis acid Al
Ⅲ. This donor-acceptor interaction could be an important thermodynamic driving force to form dual-SPO
B (
Fig. 3), which also provides insights into the mechanistic model for Ni-Al bimetallic catalysis [
40-
42]. To reveal the origin of control for dual-SPO
B, the multiple stage of SPOs transformation for mode 4 in
Fig. 1b were introduced for comparisons (Fig. S3 for detailed free energy profiles in Supporting information). Unlike the direct dehydrogenation of mode 4, transition metal Ni in redox dehydrogenation mode 6 makes the P-H bond of SPO convert to the activated Ni-H bond
via P-H oxidative addition, and then Ni-H bond proceeds a favorable reductive dehydrogenation (
Figs. 3 and
5b). There are inherent energy stabilizations between P-H RDH and Ni-H RDH (energy difference between two dotted lines). In contrast to the usual increasing energy trend in mode 4, an extra energy decreasing from 1
st to 2
nd Ni-H RDH of mode 6 seems override the nature basicity (-AlMe
2 > AlMe
3 > -AlMe), which could be attributed to different redox properties of the d orbitals of transition metal Ni. As shown in the stereo-structures in
Fig. 5b, two transition states of 1
st and 2
nd Ni-H RDH have different spatial configurations of Ni-H. The stable
TS4 of 2
nd Ni-H RDH formed a trigonal bipyramid coordination, and the apical hydride enable to interact with
dz2 orbital of Ni. While the square planar coordination can be found in the less stable
TS2 of 1
st Ni-H RDH, and the planar hydride reoccupied to the
dx2-y2 orbital of Ni. IBO analysis in
Figs. 2 and
3 can also indicate the
dx2-y2 and
dz2 orbitals of Ni operated in the dehydrogenation process, respectively. Therefore, the redox potential of Ni-H compensates the weak basicity of -AlMe
2, showing reductive basicity for the unusual trend of energy barriers. In
Fig. 5c, the closely degenerate e
g orbital (
dz2 and
dx2-y2) in trigonal-bipyramid field of dual-SPO species would fulfil efficient electron reoccupation of Ni-H and the orbital recombination with anti-bond (P=O) (BD*) which was supported by relatively low
d orbital component. That is in contrast to mono-SPO one in square-planar field (Fig. S6 in Supporting information). Moreover, the Lewis acid Al
Ⅲ interaction with SPO can not only stabilize the BD* orbital to match the
dx2-y2 orbital in energy level, but also meet symmetry-adapted
dx2-y2 orbital rather than
dz2 orbital under the dual-coordination model (Fig. S5 in Supporting information). Therefore, the Lewis acid (L) and e
g (E) orbital interactions were synergetic (S) through the SPO linker that stabilized dual-SPO model for both kinetic and thermodynamic perspectives. This LES effect is particularly efficient for reductive process (
i.e., reductive dehydrogenation) with relatively high positive NPA charge on metal center in
Fig. 5c.