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values show an agreement with the experimental observations
only if the carboxylate group is oriented to the outside of the
pillar[5]arene cavity. In this situation the nuclei (H and H ) that
Supporting Information). Significantly, only the bands associat-
ed with in-plane ring vibrations at 1391, 1022, 772, and
À1
519 cm are enhanced in the SERS spectra. This suggests
d
e
are close to the aromatic rings are more shielded, that is, they
appear at smaller chemical shifts than in the isolated 2-naph-
thoate anion (around d=2–3 ppm). However, for the opposite
orientation with the carboxylate group clearly inside the cavity,
a perpendicular orientation of the 2-naphthoate anion relative
to the gold surface, which is in agreement with the proposed
perpendicular adsorption preference of AP[5]A over the gold
À1
surface. Finally, SERS signals at 770 and 1388 cm are perfectly
1
the theoretical values of the H magnetic shieldings for the
recognized down to 1 mm. It should be pointed out as an im-
portant advantage that the detection can be performed direct-
ly in the colloidal suspension in water, which contributes to
the reliability and reproducibility of the detection.
nuclei closer to the carboxylate group would be larger than in
the isolated 2-naphthoate anion (around d=4 ppm).
So far we have proven that the AP[5]A is adsorbed onto the
quasi-spherical Au nanoparticles with the pillar[5]arene cavity
perpendicularly oriented to the metal surface. In addition, we
have also confirmed the ability of this water-soluble pillar[5]ar-
ene to bind 2NA, forming a [2]pseudorotaxane. With this infor-
mation at hand, we are ready to analyze the sensing ability of
the pillar[5]arene-stabilized gold nanoparticles towards 2NA by
SERS. On one hand, it is important to note that 2NA cannot be
detected by SERS spectroscopy using citrate-stabilized Au (or
Finally, we analyzed the possibility of detecting a polycyclic
aromatic hydrocarbon, such as pyrene, again using the AP[5]A-
stabilized Au nanoparticles in solution. PYR belongs to a family
of hazardous pollutants with a condensed benzene ring struc-
[16]
ture, which confers a very low affinity by metals. Therefore,
its detection by SERS requires the presence of an appropriate
host, that is, with strong affinity towards plasmonic surfaces
and a high selectivity for interaction with a molecule contain-
ing four benzene rings. In agreement with previous assign-
[
33]
Ag) nanoparticles, as reported in the literature, because of
its low affinity to metallic surfaces, as well as electrostatic re-
pulsions. On the other hand, 2NA presents several characteris-
tic Raman signals that do not overlap with those from AP[5]A
[16]
ments, the Raman spectrum of PYR (Figure 7A) is dominated
À1
by ring C=C stretching (1407 and 1242 cm ), ring deformation
À1
À1
(409 cm ), ring breathing (594 cm ), ring C=C stretching
À1
À1
(see the calculated Raman spectra for 2NA and AP[5]A in Fig-
(1594 and 1628 cm ), and CH bending (1067 and 1143 cm ).
Most of the signals do not overlap with those from AP[5]A (see
the calculated Raman spectra for PYR and AP[5]A in Figure S14,
the Supporting Information), therefore PYR can in principle be
detected by SERS using AP[5]A as the host molecule. Fig-
ure 7B–D shows the SERS spectra of PYR after subtracting the
AP[5]A peaks (the SERS spectra including AP[5]A contributions
are shown in Figure S15, the Supporting Information). Remark-
ably, the most intense signals in the SERS spectra correspond
to ring vibrational modes of ag symmetry (see Table S4, the
Supporting Information). Again, this can be explained if pyrene
is oriented perpendicularly to the metal surface because for
ure S12, the Supporting Information). In agreement with previ-
[
33,34]
ous assignments,
the Raman spectrum for the 2-naphthoic
acid (Figure 6A) is characterized by ring stretching (1633, 1391,
À1
À1
and 1022 cm ), CH bending (1470 cm ), ring breathing
À1
À1
(
772 cm ), and ring deformation (519 cm ). Additional vibra-
tional assignments for CH bending based on theoretical DFT
calculations can be found in the Supporting Information (see
Table S3). As shown in Figure 6, a well-defined SERS spectrum
was obtained when 2NA was added to AP[5]A-stabilized 80 nm
Au nanoparticles in water at pH above the pK (4.17) of 2NA. It
a
also confirms the complexation between 2NA and pillar[5]ar-
ene. To facilitate the analysis, Figure 6 shows the SERS spectra
after subtracting the SERS signals from AP[5]A (the SERS spec-
tra including AP[5]A contributions are shown in Figure S13, the
the a modes the Raman polarizability change would be large
g
along the molecular axis normal to the surface (see Figure S16,
[35]
the Supporting Information). Finally, SERS signals at 594 and
À4
Figure 6. A) Raman spectrum of 2NA; B–D) SERS spectra of 2NA at 10 (B),
Figure 7. A) Raman spectrum of solid pyrene; B–D) SERS spectra of pyrene
at 10 (B), 10 (C), and 10 m (D). The excitation laser line was 785 nm. In
À5
À6
À6
À7
À8
10
(C), and 10 m (D). The excitation laser line was 785 nm. In spectra B–
D, the SERS contributions from AP[5]A were subtracted.
spectra B–D, the SERS contributions from AP[5]A were subtracted.
Chem. Eur. J. 2014, 20, 1 – 7
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