The new molecules
P3RhMe3-n
(OTf)
n
are reported (n = 0−2; P3 =
MeC(CH2PMe2)3; OTf
=
OS(O)2CF3). The known
fac-(Me3P)3RhMe3
was converted to
mer-(Me3P)3RhMe3-n
Cl
n
(n =
1, 2) by cleavage with HCl in ether. X-ray photoelectron spectra
(XPS) of these were recorded,
and all except the
P3RhMe3-n
Cl
n
series afforded clean spectra. XPS were also obtained
for
the known CnRhMe3-n
X
n
(n = 0−2; X = Cl, Br, OTf; Cn =
1,4,7-trimethyl-1,4,7-triazacyclononane), CnRhX3 (X = Cl, Br),
CnRhMe(OH)(OTf), and [CnRhMe2(CO)]OTf.
An
X-ray crystal structure of P3RhMe3 is
reported, and the geometry at the metal is compared
among P3RhMe3,
(Me3P)3RhMe3, and
CnRhMe3. Core binding energies (BEs) for the
series
L3RhMe3-n
X
n
(L3 = Cn, P3) change linearly with
n for a given L3 and X. For
CnRhMe3-n
X
n
,
replacement of methyl by chloride or bromide gives similar ΔBE values
(∼0.7 eV), while
triflate-for-methyl substitution gives a much larger ΔBE (1.2 eV).
Triflate-for-methyl
substitution in
P3RhMe3-n
(OTf)
n
,
however, causes a ΔBE of only 0.8 eV. Thus, the
Rh(3d5/2)
core binding energies in these complexes change less in
triflate-for-methyl substitutions when
the P3 ancillary ligand is present than in the presence of
Cn; apparently P3 compensates for
changes in electron density at the rhodium center more effectively than
does Cn, presumably
as a result of the greater polarizability of phosphorus (softer)
compared to nitrogen (harder).
The XPS trends for these series effectively mean that
P3 makes RhIII a softer metal and
Cn
makes RhIII a harder metal.