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ing coordination ability of the ter-dentate BTP units and a supe-
rior confinement effect of the micropores, which restrict the
diffusion of the palladium NPs and their precursors from interi-
or pores to the external surface of POP-1 during the prepara-
tion of the palladium NPs. In contrast, the palladium NPs in
Pd/POP-2 are uniformly located on the external surface with
an average size of (3.3Æ0.3) nm (Figures 3d and e), which is
probably ascribed to the filling of the interior cavities by the
COOMe groups. Interestingly, the change of the functional
groups from the COOMe to the carboxylate group results in
the formation of dual-distributed palladium NPs in the interior
pores and on the external surface of POP-3 (Figures 3g and h),
and the average diameters of the palladium NPs in Pd/POP-3
are (1.6Æ0.35) and (3.5Æ0.35) nm, respectively, which are
comparable with those in Pd/POP-1 and Pd/POP-2, respective-
ly. The dual distribution of the palladium NPs in POP-3 is prob-
ably ascribed to a synergetic effect of the carboxylate groups
by electrostatic and/or coordination interactions. The size, loca-
tion, and distribution of the palladium NPs in the interior pores
and the external surface were further demonstrated by high-
annular dark-field scanning TEM (HAADF-STEM) and energy-
dispersive X-ray (EDX) mapping images of Pd/POP-1, Pd/POP-2,
and Pd/POP-3 (Figures 3c, f, and i as well as Figure S7 in the
Supporting Information).
The existing state of the surface palladium in Pd/POP-1, Pd/
POP-2, and Pd/POP-3 was investigated by X-ray photoelectron
spectroscopy (XPS). As shown in Figure 2c, the Pd 3d spectra
present two sets of doublet peaks corresponding to Pd 3d5/2
and Pd 3d3/2. The Pd 3d5/2 peaks at 335.75, 335.90, and
335.40 eV are attributed to Pd0 species of Pd/POP-1, Pd/POP-2,
and Pd/POP-3, respectively. In comparison with Pd/POP-1,
a positive shift of 0.15 eV and a negative shift of 0.35 eV was
observed for Pd/POP-2 and Pd/POP-3, respectively, which ex-
hibits that Pd0 species in Pd/POP-2 are more electron-deficient
than in Pd/POP-1 because of an electron-withdrawing effect of
the COOMe group, whereas an electron-donating effect of the
carboxylate group results in more electron-rich Pd0 species in
Pd/POP-3.[11,34] The ratio of Pd0 to PdII in Pd/POP-1, Pd/POP-2,
and Pd/POP-3 are 0.49, 0.52, and 0.41, respectively. It should
be mentioned that the Pd 3d5/2 binding energy peaks for PdII
species in Pd/POP-1, Pd/POP-2, and Pd/POP-3 shift negatively
by 0.65, 0.45, and 0.70 eV, respectively, in comparison with that
of 338.4 eV for free Pd(OAc)2,[4] the negative shift is ascribed to
the strong coordination interaction of PdII with the chelating
ter-dentate BTP units, in which election donation from BTP to
PdII makes the PdII species less electron-deficient.
In order to further confirm the interactions between the
supports and the incorporated palladium species, XPS spectra
of N 1s in the POPs and the Pd/POPs systems were implement-
ed (Figure 2d). The peaks at 399.45, 399.60, and 399.70 eV cor-
respond to the N 1s of POP-1, POP-2, and POP-3, respectively.
The peaks in Pd/POP-1, Pd/POP-2, and Pd/POP-3 are shifted to
399.65, 399.70, and 399.75 eV, respectively. The shift of the N
1s toward higher binding energies results from coordination of
nitrogen atoms to palladium,[42–44] which further suggests the
electron donation from the BTP units to the palladium species
after palladium loading.
It has been reported that the loading amount of palladium
precursors and the reduction methods may influence the struc-
tures and properties of the palladium NPs,[2] however, we
failed to obtain uniformly distributed palladium NPs even
when half the amount of Pd(OAc)2 with respect to Pd/POP-3
was used under the same conditions, no apparent variation
was observed in their TEM images (Figures 4a and d). In addi-
tion, the variation of the reduction agent of Pd(OAc)2 from
NaBH4 to H2 or N2H4·H2O has no detectable effect on the dual
distribution of the palladium NPs on the external surface of
POP-3, either (Figures 4b, e, c, and f). These results reveal that
the introduction of carboxylate groups not only can modulate
the properties of the POPs, but also exerts an important effect
on the formation and structure of the palladium NPs.
To have a clear insight into the effects of the functional
groups on the electronic properties of POP-1, POP-2, and POP-
3, the hybrid Becke three-parameter Lee–Yang–Parr (B3LYP)
density functional method in combination with the 6-311+
G(d) basis set were performed based on their model com-
pounds. As shown in Figure 5 and Table S2 in the Supporting
Information, the H, COOMe, and COOÀ groups at the BTP units
significantly influence their charge distribution. The charges of
the pyridyl nitrogen atom in POP-1, POP-2, and POP-3 are
À0.415, À0.393, and À0.438 e, respectively, which are more
negative than the nitrogen atoms in 1,2,3-triazolyl. In compari-
son with POP-1, the electron-withdrawing COOMe group in
POP-2 and the electron-donating carboxylate group in POP-3
result in a positive shift of 0.022 e and a negative shift of
0.023 e, respectively, which is consistent with the results of the
XPS analyses. The nitrogen atoms of the 1,2,3-triazolyl groups
in POP-1, POP-2, and POP-3 all possess negative charges, the
charges of the N1 and N3 atoms are almost equal, and are
more negative than that of the N2 atom. In view of the charge
density of the pyridyl nitrogen atom and the nitrogen atomic
arrangement of the 1,2,3-triazolyl group, the BTP unit prefers
to coordinate with palladium in a N3-N4-N3’ ter-dentate che-
lating mode, which is the same as those in the BTP-based co-
ordination compounds.[45–49] HOMO and LUMO analyses reveal
Figure 4. TEM images of Pd/POP-3 prepared a,d) by using half of the theo-
retical amount of Pd(OAc)2, b,e) by using H2 as a reducing agent, and c,f) by
using N2H4 as reducing agent.
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Chem. Eur. J. 2016, 22, 1 – 10
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