ChemComm
Communication
Fig. 3 TEM images of ODA capped CdSe (left), ArS–CdSe (middle), and
ArSe–CdSe (right).
on the cleavage of a phosphonate moiety on the desired ligand
for direct attachment onto the nanoparticle. We showed that this
method is applicable for both sulfur and selenium containing
ligands where established ligand exchange processes with similar
traditional ligands are difficult. Use of this method for the attach-
ment of semiconducting polymers to CdSe NPs for use in photo-
voltaic cells is currently under investigation.
Financial support is greatly appreciated from the AFOSR
FA9550-10-1-0430 and the NSF SOLAR Award DMR 1035196.
Part of this work was conducted at the University of Washington
NanoTech User Facility, a member of the NSF National Nano-
technology Infrastructure Network (NNIN). The authors would
like to thank Ryan E. Toivola for experimental assistance.
Fig. 2 (a) XPS data for S2p binding energies for ArS–CdSe (top), ArSH (center),
and ArSP (bottom); (b) photoluminescence of CdSe NPs with octadecylamine
functionalization (solid line) and quenched photoluminescence with aryl function-
alization (dashed line).
vaporizes during NP synthesis. The hexanes wash containing
ArS functionalized NPs shows no NMR signal, which indicates
cleavage of the phosphonate group ArSP, although there is a
small chance that this is due to signal broadening due to an
inhomogeneous magnetic field on the nanoparticle surface.5b
As further evidence of actual ligand attachment to CdSe as
opposed to some form of decomposition, we looked at X-ray photo-
electron spectroscopy (XPS) and photoluminescence (PL). The bottom
spectrum in Fig. 2a was measured on neat, unreacted ArSP, while the
S2p core level spectrum (center) was measured on ArSH. Due to the
low photo-ionization cross section of the S atoms13 the signal-to-noise
ratio is low, resulting in a high residuum peak fitting. Yet, it is
apparent that the peak maxima differ only marginally by about 0.3 eV,
which is expected considering the similar electronegativity of H and P.
Upon formation of the ArS-capped CdSe nanoparticles, the S2p
spectrum shown at the top of Fig. 2a indicates a shift of the core
level by B0.8 eV to higher binding energy relative to the ArSH ligand.
Considering an overall resolution of Æ0.1 eV for such measurements,
this shift is significant and can be explained as the transfer of electron
density from the sulfur atoms to the Lewis acidic Cd metal ions,
indicating the bonding of the ligand to the surface of the CdSe.14 We
also observed PL quenching with ligand attachment relative to CdSe
nanocrystals synthesized without our ligands, as can be seen in
Fig. 2b. PL quenching is expected due to the attachment of conjugated
sulfur containing ligands to the surface of CdSe because the aromatic
p-electrons can act as efficient acceptors for photogenerated holes,
thus hindering the radiative recombination process.6
This in situ ligand attachment process is not limited to ligands
containing a sulfur–phosphonate bond. We found similar NMR and
XPS results when S was replaced by Se and ArSeP ligands were
attached to CdSe NPs in an analogous fashion, as can be seen in
Fig. S6 and S7 in the ESI.† However, with the attachment of the
ArSeP ligands, we found that we were not able to maintain size and
shape control as we were previously able to do with attachment of
the ArSP ligands under the same conditions, as can be seen in
Fig. 3. This loss of size and shape control is attributed to the greater
reactivity of the Se-containing ligands. Others have previously shown
a lack of control with highly reactive ligands.15
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In summary, we report here a novel procedure for organic/
CdSe NP hybrid material synthesis. The process developed relies
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c
This journal is The Royal Society of Chemistry 2013
Chem. Commun., 2013, 49, 1321--1323 1323