C O M M U N I C A T I O N S
with a silylated Tb-EDTA monoamide derivative, 3′-Tb-EDTM
Scheme 1). Tb3 ions and molecular Tb complexes have been
+
10
11
(
used as sensitive luminescence probes for anthrax and other bacterial
spores by complexing to DPA, which constitutes up to 15% of the
spores’ dry mass. Upon excitation at 278 nm, 3′-Tb-EDTM only
gave Eu luminescence because the Tb-EDTM moiety is essentially
nonemissive. As DPA was added to an ethanolic dispersion of 3′-
Tb-EDTM, the Tb luminescence became clearly visible due to the
formation of the Tb-EDTM-DPA complex. The Tb luminescence
signal provides a sensitive probe for DPA detection, while the Eu
emission from the NMOF core acts as noninterfering internal
calibration. As shown in Figure 2d, the relationship between the
ratio of Tb to Eu emission intensities and DPA concentration
displayed normal saturation behavior. At low DPA concentrations,
the ratio of signal intensities increased linearly; however, the ratio
of intensities began to level off as the Tb-EDTA complexes became
coordinatively saturated with DPA. The DPA detection limit for
this system was estimated to be ∼48 nM. Such a ratiomeric sensing
scheme works equally well in a Tris buffer solution and is able to
selectively detect DPA in the presence of biologically prevalent
interferences such as amino acids (Supporting Information).
In summary, we have developed a general method to coat
NMOFs with silica shells of variable thickness. These shells increase
NMOF core stability and allow for the controlled release of metal
constituents. Silica-coated NMOFs were further functionalized for
the detection of DPA, an important molecular marker in spore-
producing bacteria. Owing to the tunability of NMOF composition
and morphology, the present approach should allow for the synthesis
of novel core-shell hybrid nanostructures for future imaging,
sensing, and drug delivery applications.
Figure 2. TGA curves for 1-3 synthesized at (a) W ) 5 and at (b) W )
5 (black ) 1; blue ) 2; red ) 3 with a 2-3 nm silica shell; green ) 3
with an 8-9 nm silica shell). (c) Time-dependent dissolution curves for 1
red) and 3 (black) with an 8-9 nm silica shell at pH ) 4 and 37 °C. (d)
Dependence of the ratio of Tb to Eu emission intensities for 3′-Tb-EDTM
on DPA concentration (red ) 544 nm/592 nm, black ) 544 nm/615 nm).
The inset shows the linear relationship at low [DPA].
1
(
The compositions of 2 and 3 were further established by TGA
(Figure 2a,b) and powder X-ray diffraction (PXRD). TGA results
showed that 2 had a slight increase of the total weight loss over
that of 1 as a result of the PVP coating (5.5% for W ) 5 and 1.5%
for W ) 15). In contrast, the weight loss for 3 decreased
2
significantly due to the presence of a SiO coating. For 3 synthesized
at W ) 5, a 2-3 nm silica coating led to a 9.6% reduction in weight
loss, whereas an 8-9 nm coating of silica reduced the total weight
loss by 28.5%. For 3 synthesized at W ) 15, a 2-3 nm silica
coating led to a 9.4% reduction in weight loss, whereas an 8-9
nm coating of silica reduced the total weight loss by 25.7%. The
smaller changes to total weight loss for 2 and 3 synthesized at W
Acknowledgment. We acknowledge financial support from
NSF and NIH grants. W.J.R. thanks NSF for a graduate research
fellowship, and W.L. is a Camille Dreyfus Teacher-Scholar.
)
15 were consistent with the reduced surface areas for larger
Supporting Information Available: Experimental procedures and
particles. PXRD studies showed that 2 and 3 exhibited the same
pattern as macroscopic 1, further proving the presence of the
crystalline NMOF core in both PVP- and silica-coated 1. Interest-
ingly, the NMOF core of 3 could be completely removed (via
dissolution) at low pH to afford hollow silica shells with varied
thickness and aspect ratios (Figure 1h). Since the morphologies of
NMOFs can be controlled by exploiting the energetics of different
crystallographic faces, we believe the present approach can be used
to produce interesting nanoshells that are not accessible with
presently available templates.
We have also examined the stabilizing effect of an 8-9 nm silica
shell on the NMOF core. Figure 2c shows the dissolution curves
for 1 and 3 when dialyzed against water at 37 °C. The dissolution
curves for both 1 and 3 at pH ) 4 can be modeled as a zeroth-
order rate law with an apparent rate constant of 0.143 and 0.084
µM/h, respectively. The silica shell of 3 has thus stabilized the
NMOF core against dissolution. A similar stabilizing effect of the
silica shell was also observed at pH ) 5, with an apparent rate
constant of 0.085 and 0.044 µM/h for 1 and 3, respectively. These
results indicate that the rates of cargo release from such core-
shell nanostructures can be readily controlled, presumably by taking
advantage of slow diffusion of metal and organic constituents
through the silica shell.
1
7 figures. This material is available free of charge via the Internet at
http://pubs.acs.org.
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2 2 2
tures, we have prepared Eu-doped Gd(BDC)1.5(H O) @SiO nano-
particles (3′) at W ) 5 and further functionalized the silica surface
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