Binuclear Pd(II) and Pt(II) complexes
supported by rac-dpmppm (bis[(diphenylphosphinomethyl)phenylphosphino]methane)
in
a triply-bridged Z-form, [M2Cl4(rac-dpmppm)] (M = Pd (3a), Pt (3b)), readily reacted with 2,6-xylyl isocyanide (XylNC) in
the presence of NH4PF6 to afford [M2Cl2(rac-dpmppm)(XylNC)2](PF6)2 (M = Pd (4a), Pt (4b)), in which each metal center accommodates one isocyanide ligand
at the trans position to the inner P atom of dpmppm.
Similarly, treatment of 3a and 3b with axially
chiral (R/S)-1,1′-binaphthyl-2,2′-bisisocyanide
(rac-Binac) in the presence of NH4OTf
gave cyclic tetranuclear complexes, [{M2Cl2(rac-dpmppm)(rac-Binac)}2](OTf)4 (M = Pd (5), Pt (8)), where two
{M2Cl2(rac-dpmppm)}2+ fragments are connected by two rac-Binac ligands
through chirality sorting of (R*,R*)-dpmppm and (R*)-Binac. Complex 5 could be transformed into
the halide exchanged tetranuclear complexes, [{Pd2X2(rac-dpmppm)(rac-Binac)}2](OTf)4 (X = Br (6), I (7)), to show that the rectangular arrangement of four Pd(II) ions
is elongated by repulsive interaction between halide ligands. By using
(R)- and (S)-Binac, enantiopure
Pd4 complexes, [{Pd2Cl2((R*,R*)-dpmppm)((R*)-Binac)}2](OTf)4 (5
RR/R
and 5
SS/S
), were successfully isolated as pure crystalline forms, from which
enantiopure (R,R)- and (S,S)-dpmppm
were obtained by treatment with NaCN aqueous solution. Namely, optical
resolution of rac-dpmppm was established through
the tetranuclear Pd complexes, which is the first example for methylene-bridged
polyphosphines, R2P(CH2PR)
n
CH2PR2 (n > 0). Furthermore,
chiral octapalladium chains, [Pd8((R*,R*)-dpmppm)4(NCCH3)2](BF4)4 (2
RR
and 2
SS
), were synthesized by reacting enantiopure P-chiral dpmppm with [Pd2(CH3CN)6](BF4)2 and [Pd2(dba)3]·C6H6 and were characterized by
spectroscopic and X-ray crystallographic analyses, to determine the
absolute configurational structures. The Pd8 chains are
the longest enantiopure chiral single-metal-atom chains structurally
characterized, thus far, and the electronic structures were examined
on the basis of DFT calculations of 2
RR
.