C O M M U N I C A T I O N S
hot-spots in Figure 1d. Strong SERS signals observed at spots I,
II, and III were generated by tetramer, trimer, and dimer NPs,
respectively. Although the SEM image (Figure 1e) also revealed
another Ag aggregate located at the lower left of the cell, careful
examination of this cluster with SEM showed that the Ag cluster
is actually embedded inside the cell. Raman spectra taken from
this region do show enhancement, although much weaker in
intensity (∼50-fold) compared with those aggregates located on
the cell surface. Moreover, repeated cell surface labeling with Ag-
NP-1 indicated that only nanoparticle aggregates (dimers or greater)
showed measurable SERS signals. Generally, the SERS enhance-
ment factor is about 1010 (see Supporting Information).
Theoretical calculations have shown that SERS enhancement
factors from isolated NPs are orders of magnitude smaller than those
of aggregated NPs.9 The SERS enhancement factor of a dimerized
NP increases dramatically when the molecule of interest is situated
in the interstitial gap of the dimer NPs,9,10 implying that enhance-
ment depends strongly on the interstitial gap between the NPs. With
an interstitial gap of ∼5 nm, the SERS enhancement factor can
exceed 6 orders of magnitude and 10 orders of magnitude with a
1 nm interstitial gap.11 Trimers and other smaller NP aggregates
can be treated as ensembles of coupled dimer systems and therefore
can produce extremely intense SERS hot-sites provided sufficiently
small interstitial gaps are present. Although single NPs are capable
of field enhancement, their SERS intensity is simply too weak to
be observed in our imaging experiments.
We also observed that aggregated NPs exhibit strong polarization
anisotropy. Particles identified in the SEM images labeled as spots
I, II, and III (Figure 1e) all have their interparticle axes oriented
largely parallel to the incident electric field. This relationship is
necessary to achieve a capacitive field enhancement and hence
generate intense SERS hot-sites.4,10 If the incident light polarization
is perpendicular to the interparticle axes of the aggregated NPs,
the exclusion of the field between the NPs results in no enhancement
(see Supporting Information).
As the Raman images were obtained by rastering cells under a
tightly focused incident beam, light-induced damage is a legitimate
concern. To investigate this problem, we observed SEM images of
several cells before and after Raman imaging (Figure 2a). The
Raman and SEM image of a representative cell showed excellent
correlation between the locations of SERS and aggregated Ag-NP-
1. The same cell was examined under SEM after Raman imaging.
We observed localized rupturing of the cell membrane under several
aggregated Ag-NP-1 (Figure 2c,d) and a NP monomer (Figure 2b).
These results indicated that damage at NP aggregates was the most
extensive. Supporting this was the finding that, when we reduced
the imaging power density by 1 order of magnitude, no detectable
membrane damage was observed. Similar NP-induced photothermal
effects to cells have been reported12 and often result in irreparable
damage to cells.
In summary, we have demonstrated imaging of membrane
proteins on cells using a cyano-labeled SERS probe. Observed
SERS hot-sites correlate well with small aggregated NPs. Further-
more, the strongest SERS signals originate from aggregates oriented
in the appropriate direction with respect to the incident laser
polarization. These observations are critical for the design of future
molecular imaging agents for SERS imaging of cells and tissues.
Fortuitously, many cell surface receptors function as clusters which
may help to facilitate NP aggregation and orientation in cellular
Figure 2. (a) SEM image of a cell. Upper right inset: magnification of a
group of aggregated NPs. The scale bar is 200 nm. Lower left inset: the
corresponding Raman intensity image of the same cell obtained with a power
density of 105 W/cm2. Laser-induced damage to the cell is shown in (b)
the monomer (blue circle in a), (c) the aggregates, and (d) a pair of dimers.
and tissue imaging experiments.13 We are currently pursuing such
imaging studies.
Acknowledgment. We thank Prof. Alice Ting at MIT for
providing biotin ketone, as well as the AP-CFP-TM and BirA
plasmids. We gratefully acknowledge the help of Mr. Jeff Fraser
for SEM imaging, and Dr. Jean Lapointe for fabricating the
patterned Si substrate.
Supporting Information Available: Experimental details and
information on polarization anisotropy. This material is available free
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