Nanojars are a class of supramolecular coordination complexes based on pyrazolate, Cu2+, and OH- ions that self-assemble around highly hydrophilic anions and serve as efficient anion binding and extraction agents. In this work, the synthesis, characterization, and photophysical properties of pyrene-functionalized fluorescent nanojars are presented. Three pyrene derivatives, 4-(pyren-1-yl)pyrazole (HL1), 4-(5-(pyren-1-yl)pent-4-yn-1-yl)pyrazole (HL2), and 4-(3-(pyrazol-4-yl)propyl)-1-(pyren-1-yl)-1,2,3-triazole (HL3), and the corresponding nanojars were synthesized and characterized using nuclear magnetic resonance spectroscopy and mass spectrometry. Electronic absorption, steady-state, and time-resolved fluorescence measurements were carried out to understand the interaction between the pyrene fluorophore and copper nanojars. Optical absorption measurements have shown minor ground state interaction between the fluorophore and nanojars. The fluorescence of pyrene is significantly quenched when attached to nanojars, suggesting strong contribution from the paramagnetic Cu2+ ions. Significant static quenching is observed in the case of L1, when pyrene is directly bound to the nanojar, whereas in the case of L2 and L3, when pyrene is attached to the nanojars using flexible tethers, both static and dynamic quenching are observed.
Nanojars are a class of supramolecular coordination complexes based on pyrazolate, Cu2+, and OH- ions that self-assemble around highly hydrophilic anions and serve as efficient anion binding and extraction agents. In this work, the synthesis, characterization, and photophysical properties of pyrene-functionalized fluorescent nanojars are presented. Three pyrene derivatives, 4-(pyren-1-yl)pyrazole (HL1), 4-(5-(pyren-1-yl)pent-4-yn-1-yl)pyrazole (HL2), and 4-(3-(pyrazol-4-yl)propyl)-1-(pyren-1-yl)-1,2,3-triazole (HL3), and the corresponding nanojars were synthesized and characterized using nuclear magnetic resonance spectroscopy and mass spectrometry. Electronic absorption, steady-state, and time-resolved fluorescence measurements were carried out to understand the interaction between the pyrene fluorophore and copper nanojars. Optical absorption measurements have shown minor ground state interaction between the fluorophore and nanojars. The fluorescence of pyrene is significantly quenched when attached to nanojars, suggesting strong contribution from the paramagnetic Cu2+ ions. Significant static quenching is observed in the case of L1, when pyrene is directly bound to the nanojar, whereas in the case of L2 and L3, when pyrene is attached to the nanojars using flexible tethers, both static and dynamic quenching are observed.
Nanojars (NJs) constitute
an interesting class of cyclic coordination
oligomers based on the neutral {cis-CuII(μ-OH)(μ-pz)} (pz = pyrazolate anion or a derivative)
repeating unit (Figure ).[1] Highly hydrophilic oxyanions, such
as carbonate, sulfate, phosphate, and arsenate, template the self-assembly
of NJs of the formula [anion⊂{Cu(μ-OH)(μ-pz)}]2– (Cu; n = 26–33).[2−7] Each member of this series of oligomerization isomers is composed
of three [{Cu(μ-OH)(μ-pz)}] (m = 6–14, except 11) metallamacrocycles,
strongly held together by an intricate network of hydrogen bonds and
Cu···O interactions. As the NJs self-assemble, a hydrophilic
cavity lined by a multitude (26–33) of O–H hydrogen
bond donors forms at their center, which incarcerates the templating
oxyanion. Consequently, NJs have been developed into highly efficient
anion-extracting agents,[8] capable of binding
trace amounts of oxyanions and transferring even the most hydrophilic
ones from water into long-chain aliphatic hydrocarbon solvents.[9] Selective binding of oxyanions has recently been
achieved by tethering pairs of pyrazolate ligands together.[10,11]
Figure 1
Example
of a NJ crystal structure (top- and side-views). Shown
here is [CO3 ⊂ {CuII(μ-OH)(μ-pz)}6+12+9]2– (H-atoms are omitted for clarity).
Example
of a NJ crystal structure (top- and side-views). Shown
here is [CO3 ⊂ {CuII(μ-OH)(μ-pz)}6+12+9]2– (H-atoms are omitted for clarity).Aiming at detecting NJs using fluorescence and
ultimately developing
NJ-based sensors for oxyanions, we pursued the synthesis and characterization
of fluorescent NJs. Various polar substituents (including nitro, amine,
aldehyde, carboxylate) as well as acidic groups (phenol, thiol, carboxylic
acid) interfere with NJ formation. Therefore, we opted for pyrene
as the fluorescent label, an aromatic hydrocarbon with no polar or
acidic groups yet a very versatile fluorescent moiety. Indeed, pyrene-based
fluorescent tags have been used in various coordination complexes,[12] metal–organic frameworks,[13,14] and self-assembled nanomaterials,[15] in
fluorescent sensors for the detection of explosives[16] or transition metal ions such as Cu2+,[17] Zn2+,[18] Hg2+,[19] and Fe3+,[20] in luminous molecular liquids,[21] surfactant aggregates,[22,23] and dendrimers.[24] Pyrene-based materials
are also valuable in organic electronics,[25−28] photoswitchable nonlinear optical[29] and electroluminescent materials,[30] light-harvesting antenna systems,[31−33] photoinitiators of polymerization[34] and
other light-induced reactions,[35,36] molecular receptors,[37−40] and electrocatalysis.[41] Pyrene is also
used for imaging biological systems[42−45] and for photodynamic therapy.[46] The methods of functionalization of pyrene to
prepare luminescent materials have been reviewed.[47] However, very few studies have focused on the excited-state
interactions between fluorescent dyes and supramolecular inorganic
nanomaterials.[48]Herein, we present
the synthesis and characterization of three
novel pyrene-functionalized pyrazole ligands, 4-(pyren-1-yl)pyrazole
(HL1), 4-(5-(pyren-1-yl)pent-4-yn-1-yl)pyrazole (HL2), and 4-(3-(pyrazol-4-yl)propyl)-1-(pyren-1-yl)-1,2,3-triazole
(HL3) (Scheme ). In HL1, the fluorescent tag is directly bound
to the pyrazole moiety; therefore, the fluorophore is conjugated with
the Cu2+ centers in NJs via the pyrazole unit, and its
position relative to the NJ is rigid. In contrast, in HL2 and HL3, the fluorescent tag is attached to the pyrazole
moiety via a propylene chain (and a −C≡C– or
triazole group in HL2 and HL3, respectively),
which allows for flexibility of the fluorophore relative to the NJ
and disrupts conjugation between the fluorophore and the Cu2+ centers. Three different ways of synthesizing fluorescent NJs based
on these ligands are described. Electrospray-ionization mass spectrometry
(ESI-MS), nuclear magnetic resonance (NMR), optical absorption, steady-state
and time-resolved fluorescence measurements were carried out to characterize
the novel NJs and to monitor their interaction with the attached pyrene
dye.
Scheme 1
Synthesis of the Fluorescent Pyrazole Ligands
Results and Discussion
Synthesis of the Fluorescent Pyrazole Ligands
Our previous
investigations had established that steric influences from bulky substituents
at the 3-position of pyrazole ligands can hinder the self-assembly
of NJs, whereas functionalization at the 4-position does not interfere
with NJ formation.[9] Thus, the simplest
fluorescent pyrazole ligand was synthesized by directly attaching
pyrene to the 4-position of the pyrazole moiety (Scheme ). 4-Pyrazoleboronic acid pinacol
ester was first protected with a tetrahydropyranyl (THP) group (Figures S1 and S2), followed by a Suzuki–Miyaura
coupling with 1-bromopyrene. The resulting intermediate was deprotected
and the product was purified by flash chromatography to give HL1 in 50% overall yield (Figures S3 and S4).We were also interested in developing appropriately
functionalized pyrazole ligands as an avenue to constructing NJs that
have potential to be functionalized both pre- and post-synthetically.
We identified 4-(pent-4-yn-1-yl)pyrazole as a suitable starting point
for our studies, which combines several desired features: (1) the
reactive terminal alkyne functionality allows for the installation
of pyrene moieties; (2) the alkyne group is tolerated during NJ self-assembly;[49] (3) the propylene unit between pyrazole and
the alkyne prevents π-electron conjugation between the pyrazole
and the pyrene moieties, which might lead to diminishing of fluorescence
intensity. This compound has been previously prepared from 4-(3-hydroxypropyl)pyrazole
by first converting the hydroxyl group to the primary bromide using
phosphorus tribromide and subsequently performing a nucleophilic substitution
reaction with sodium acetylide to give the alkyne.[49]A terminal alkyne can be directly coupled to pyrene
using a Sonogashira
reaction. Thus, a coupling reaction was carried out using the THP-protected
4-(pent-4-yn-1-yl)pyrazole and 1-bromopyrene (Scheme ). Using Pd(PPh3)4 as
a catalyst produced the desired product along with ∼16% of
Glaser-type homocoupled di-alkyne. Replacing the catalyst with Pd(PPh3)2Cl2 reduced the amount of the side
product to ∼4%. Deprotection and purification by flash chromatography
afforded HL2 in 22% yield over two steps (Figures S5 and S6).The copper catalyzed
azide–alkyne cycloaddition “click”
reaction is also a convenient method to install pyrene-based fluorophores
on larger molecular structures containing an alkyne functionality.
Coupling of THP-protected 4-(pent-4-yn-1-yl)pyrazole with 1-azidopyrene
was carried out using click chemistry (Scheme ). The Cu+ catalyst was prepared in situ by the reduction of Cu2+ using sodium
ascorbate. The resulting crude product was deprotected using concentrated
sulfuric acid in ethanol and the product was purified by dissolving
in minimal amount of chloroform and precipitating with hexanes. Filtration
gave the pure HL3 in 47% yield over two steps (Figures S7 and S8).
Synthesis of Fluorescent
NJs by Self-Assembly Using Pyrene-Labeled
Pyrazole Ligands
NJs Based on L1
The
synthesis of homoleptic
NJs based solely on a given pyrene-labeled ligand was carried out
by self-assembly using a 1:1:2:1 molar mixture of ligand (HL1, HL2, or HL3), Cu(NO3)2, NaOH, and Na2CO3 in tetrahydrofuran
(THF) (Scheme , Method
A). With HL1, Cu27 and Cu29 NJs
of the formula [CO3⊂{Cu(OH)(L1)}]2– (n = 27, m/z 4726; n = 29, m/z 5074) are observed by
ESI-MS(−) (Figure S9). Compared
to unsubstituted NJs, the signal intensity of ESI-MS(−) is
very weak indicating poor ionization efficiency, attributable to the
large size and hydrophobicity of the pyrene-decorated NJs. The 1H NMR spectrum of the NJ mixture displays peaks in the 20–40
ppm window that are consistent with previous observations for NJs.[4,5] The signals of the chemically equivalent pyrazole protons in the
3- and 5-positions of both Cu27 (Cu6+Cu12+Cu9) and Cu29 (Cu8+Cu13+Cu8) NJs are significantly downfield shifted
compared to free pyrazole, due to the presence of paramagnetic Cu2+ ions. The extent of these shifts is temperature-dependent,
as confirmed by variable temperature 1H NMR studies in
the 25–140 °C range (Figure S10). At 25 °C, the spectrum shows four broad distinguishable peaks
at 30.3 (Cu6-ring), 27.1 (Cu8-ring), 22.4 (Cu12-ring), and 21.2 ppm (Cu13-ring). Increasing temperatures
lead to the sharpening of these peaks as the magnetic moment of the
copper complex decreases and reveal a new peak at ∼34.0 ppm
(Cu9-ring) at 50 °C which was too broad to be observable
at 25 °C. As in the [CO3⊂{Cu(OH)(pz)}]2– (n = 27, 29)
NJs studied before,[4,5] the pyrazole protons in the Cu9-ring of the Cu27 NJ are the most sensitive to
temperature changes as the corresponding peak shifts upfield by over
5 ppm units on going from 25 to 140 °C in a DMSO-d6 solution. Meanwhile, the peaks corresponding to the
Cu6- and Cu12-rings of the Cu27 NJ,
as well as the Cu8- and Cu13-rings of the Cu29 NJ experience much smaller shifts of less than 0.6 ppm units.
Scheme 2
Different Methods of Synthesizing Fluorescent NJs (Only Cu27 is Shown); In Method A, All Pyrazole Moieties of the NJ are Substituted
with Pyrene (Only Nine Substituents Are Shown for Clarity); In Method
B, NJs with Varying Numbers of Substituents (Depending on the pz/Fluorescent
Ligand Ratio) Are Obtained; For Method C, an Example with Two Substituents
Is Shown
Heteroleptic NJs synthesized
with a 1:1 molar mixture of pyrazole
(Hpz) and fluorescent ligand HL1 display a statistical
distribution of species consisting primarily of Cu27 NJs
[CO3⊂Cu27(OH)27(L1)(pz)27–]2– (x = 3–19, m/z 2323–3925), as shown by ESI-MS(−)
(Figure S11). The ionization efficiency
of these heteroleptic NJs is drastically improved compared to those
containing only L1 as the ligand.
NJs Based
on L2
The synthesis of homoleptic
NJs based on L2 proceeded similarly to the one using L1. However, these very large and hydrophobic NJs do not ionize
sufficiently to be properly characterized by ESI-MS. While some low-intensity
peaks could be discerned from the background noise in the expected
mass region for the corresponding homoleptic NJs, unequivocal assignments
could not be performed. On the other hand, heteroleptic NJs [CO3⊂Cu(OH)(L2)(pz)]2– (n = 27, x = 4–13, m/z 2556–3754; n = 29, x = 7–12, m/z 3103–3769; n = 31, x = 9–15, m/z 3517–4316) could be observed by ESI-MS(−)
if a 1:1 molar mixture of pyrazole and HL2 was used for
the synthesis. In the NJ mixture obtained, Cu27 species
are the major components; smaller amounts of Cu29 and Cu31 NJs are also observed (Figure S12). Although the ionization efficiency of these assemblies is significantly
less than that of NJs containing only unsubstituted pyrazole, the
mass spectrum has a sufficient signal-to-noise ratio to clearly distinguish
and identify these species.
NJs Based on L3
Attempts to obtain homoleptic
NJs based on L3 yielded brown, insoluble solids instead
of blue-green NJs. The triazole functionality in L3 is
also a possible coordination site for copper which can lead to the
formation of coordination polymers. This assumption is consistent
with previous studies which showed that NJs do not form with pyrazole
ligands containing additional coordinating functional groups.[9] Contrary to L1 and L2, no NJs could be obtained with pyrazole/L3 mixtures
in 1:1 or 6:1 molar ratios. Instead, unidentified copper-containing
species with m/z < 1000 were
observed in the ESI-MS in both cases. A mixture of pyrazole and L3 in a 19:1 molar ratio, however, did allow the formation
of NJs (Figure S13). Thus, the [CO3⊂Cu(OH)(L3)(pz)]2– (n = 27, x = 1–4, m/z 2178–2642; n = 31, x = 1–4, m/z 2473–2937)
species observed in the corresponding ESI-MS(−) spectrum indicate
that L3 is tolerated on NJs in small numbers (up to four L3 ligands per NJ). According to the statistical distribution[9,49] of the pyrene-functionalized ligand, unsubstituted NJs are also
observed in the mixture.
Synthesis of Fluorescent
NJs by “Click” Reaction
between Alkyne-Functionalized NJs and 1-Azidopyrene
Post-synthetic
functionalization was performed on alkyne-substituted NJs using the
Cu+ catalyzed azide–alkyne Huisgen cycloaddition
(“click”) reaction.[50,51] In most click
reactions, the Cu+ catalyst is generated in situ by reducing Cu2+ with an excess of sodium ascorbate.
This prevents Glaser-type oxidative homocoupling products of alkynes.
To prevent the possible reduction of Cu2+ ions in NJs by
ascorbate, we opted for the use of CuI as the catalyst. Furthermore,
because we had observed that the coupled product (L3)
is only tolerated on NJs in small amounts, NJs prepared with a 90:10
molar ratio of pyrazole and 4-(pent-4-yn-1-yl)pyrazole were used for
this study (Figure S14).Using THF
as a solvent, NJs containing up to three pyrene groups were observed:
[CO3⊂Cu(OH)(L3)(4-pentynylpyrazole)(pz)]2– (n = 27, x = 1, y = 0–2, m/z 2178–2244; n = 31, x = 1–3, y = 0–2, m/z 2473–2848) (Figure S14b). A significant amount of NJs containing unreacted
alkyne moieties remained. To test whether this is due to the poor
solubility of CuI in THF, we carried out the reaction in acetonitrile
(ACN) which is a good solvent for the catalyst. In this case, a dark-blue
precipitate formed in the blue reaction mixture. Its blue color and
its solubility in THF suggest that this product consists of NJs with
multiple pyrenyl-triazole substituents. The increasing hydrophobicity
of the assembly with increasing number of coupled ligands makes them
gradually less soluble in ACN. Concomitantly, the mother liquor contained
uncoupled NJs and those containing only one L3 ligand
(Figure S14c). In an attempt to prevent
the precipitation of the larger assemblies as well as to dissolve
the catalyst, we also conducted the reaction in a 1:1 mixture of THF
and ACN. Most of the alkyne functionalities have reacted in this case;
however, the abundances of the NJs containing pyrene-coupled ligands
is lower than expected in the corresponding ESI-MS(−) spectrum,
likely due to decreased ionization efficiency of the complexes containing
multiple L3 ligands (Figure S14d). Nevertheless, these experiments clearly demonstrate that NJs can
be functionalized post-synthetically.
Synthesis of NJs for Photophysical
Studies
Fluorescence
studies of NJs were hampered by trace amounts of residual, free fluorescent
ligand. Because purification of NJs containing large numbers of fluorescent
ligands proved to be difficult, we employed a mixture of pyrazole
(Hpz) and fluorescent ligand (HL1, HL2 or
HL3) in a 19:1 molar ratio (5 mol % fluorescent ligand)
to obtain NJ mixtures free of unbound ligand, suitable for photophysical
studies. Because only a small amount of fluorescent dye was employed
relative to pyrazole, it was expected that only one or two dye molecules
would be present per NJ. The corresponding ESI-MS(−) spectra,
shown in Figures S15–S17, confirm
the expected results. Some of the NJs in the mixture do not contain
any dye, which is typical for mixtures obtained by statistical distribution
of ligands.[9,49] Also, in the case of L2 and L3, small amounts of NJs with an additional allyl
substituent are observed. This is due to the presence of trace amounts
of 4-allylpyrazole byproduct in the 4-(pent-4-yn-1-yl)pyrazole precursor
used in the synthesis of L2 and L3. This
impurity is very difficult to remove completely, and as shown before,
even trace amounts are drastically amplified upon incorporation into
large assemblies, such as NJs.[49] Fortunately,
the presence of traces of allyl-substituted NJs is not a concern for
studying the fluorescence of pyrene-functionalized NJs nor is the
presence of unfunctionalized NJs, as neither contain fluorescent moieties.
These fluorescent NJ samples, used for the photophysical measurements
described below, are denoted L1-NJ, L2-NJ,
and L3-NJ.
Photophysical Studies
The main focus
of the photophysical
studies described below is understanding how the spacing between the
fluorophore and the NJ influences the optical properties of the assembly.
To that end, photophysical properties of the synthesized fluorophores
and NJ-bound fluorophores were studied using electronic absorption,
steady-state and time-resolved fluorescence measurements. Figure shows the normalized
absorbance and fluorescence spectra of HL1, HL2 and HL3 in ACN. The corresponding absorption and fluorescence
maxima are presented in Table . All synthesized pyrene derivatives have extinction coefficients
greater than 104 L mol–1 cm–1, indicating the π–π* nature of the lowest excited
state. HL2 and HL3 show pronounced vibrational
features in their absorption spectra similar to the parent, unsubstituted
pyrene molecule, whereas these spectral features are diminished in
HL1. The absorption maximum of HL3 (341
nm) is close to that of pyrene (343 nm), whereas the ones of HL1 and HL2 are shifted to 349 and 359 nm, respectively.
The red shifted absorptions suggest extended conjugation in the latter
molecules.
Figure 2
Normalized absorption and fluorescence spectra (after excitation
at 350 nm) of the pyrene derivatives HL1, HL2 and HL3 in ACN (8.4 × 10–6,
6.0 × 10–6 and 6.4 × 10–6 M, respectively).
Table 1
Photophysical
Properties of the Synthesized
Pyrene Derivatives
system
λabsmax (nm)
λemmax (nm)
quantum yield
HL1
349
388
0.26
HL2
359
381
0.08
HL3
341
385
0.085
Normalized absorption and fluorescence spectra (after excitation
at 350 nm) of the pyrene derivatives HL1, HL2 and HL3 in ACN (8.4 × 10–6,
6.0 × 10–6 and 6.4 × 10–6 M, respectively).All three
pyrene derivatives show a vibrational structure in their
fluorescence spectra and the fluorescence maxima are near 385 nm.
Fluorescence quantum yields were determined using 1,4-bis(2-methylstyryl)benzene
as standard and are provided in Table . HL1 shows a fluorescence quantum yield
of 0.26 while diminished fluorescence quantum yields were observed
for HL2 and HL3 indicating the presence
of faster non-radiative deactivation pathways in these systems.Figure A shows
the absorption spectra of HL1 and L1-NJ
(prepared as described above). Also, shown in this figure is the absorption
spectrum of the non-functionalized NJ based on the parent pyrazole
ligand (denoted pz-NJ), which displays the same absorbance maximum
at 600 nm as the dye-functionalized NJ. An increased absorbance below
400 nm is observed for L1-NJ, indicating the contribution
of L1. The absorption of L1 attached to
the NJ was determined by subtracting the absorption spectrum of pz-NJ
from the one of L1-NJ and is shown in the inset of Figure A. It is apparent
that the absorption spectrum of L1 slightly broadened
when bound to the NJ, indicating electronic interaction between L1 and the NJ. Similar analyses were carried out for L2 (Figure B) and L3 (Figure C). In these latter cases, the results indicate a negligible
ground state interaction between pyrene and NJs, and the vibrational
features of pyrene are retained even when the dyes are bound to the
NJ. These result are in agreement with the fact that the dyes are
tethered to the NJ by spacers that prevent through-bond electronic
coupling.
Figure 3
Optical absorption spectra in ACN of free and NJ-bound dyes (A) L1, (B) L2 and (C) L3 (5.9 ×
10–6, 8.4 × 10–6 and 6.4
× 10–6 M, respectively), along with the absorption
spectrum of pz-NJ without dye. Spectra of the free dye and pz-NJ were
normalized to that of the NJ-bound dye at 600 nm. Insets show the
absorbance of the free dye compared to the one of the NJ-bound dye
(determined by subtracting the absorbance of the pz-NJ).
Optical absorption spectra in ACN of free and NJ-bound dyes (A) L1, (B) L2 and (C) L3 (5.9 ×
10–6, 8.4 × 10–6 and 6.4
× 10–6 M, respectively), along with the absorption
spectrum of pz-NJ without dye. Spectra of the free dye and pz-NJ were
normalized to that of the NJ-bound dye at 600 nm. Insets show the
absorbance of the free dye compared to the one of the NJ-bound dye
(determined by subtracting the absorbance of the pz-NJ).To probe the excited state interaction between pyrene and
NJ, steady-state
fluorescence measurements were carried out. Figure A shows the fluorescence spectra of HL1 and L1-NJ dissolved in ACN. The fluorescence
of L1-NJ was corrected for the absorbance of L1 on the NJ. It is evident that the fluorescence of L1 is quenched 6.3-fold upon binding to the NJ. The inset of Figure A shows the normalized
fluorescence spectra of L1 and L1-NJ. No
noticeable shift in the fluorescence spectrum of L1 is
observed except that there is a strong fluorescence quenching. Similar
analyses were carried out for L2 (Figure B) and L3 (Figure C). Again, the fluorescence
of the dyes is significantly quenched (25- and 19-fold for L2 and L3, respectively), while only slight changes are
observed in the features of the fluorescence spectra. The observed
fluorescence quenching is explained by the proximity of the fluorophore
to the paramagnetic Cu2+ ions in the NJ. However, it is
interesting to note that the fluorescence quenching is significantly
greater for L2 and L3 than for L1, which is directly bound to the NJ. This indicates that in addition
to enhanced intersystem crossing, dynamic quenching is also present.
To rule out the presence of free pyrene dyes in solution and to prove
that quenching is associated solely with pyrenes bound to NJs, fluorescence
measurements were carried out on 1-bromopyrene at increasing concentrations
of pz-NJs (Figure S18). No fluorescence
quenching was observed even at significantly elevated concentrations
of pz-NJs, confirming that the quenching is arising only when the
pyrene is bound to the NJ. Also, to verify that the fluorescence of
the dyes is restored when the NJ is broken down, fluorescence measurements
were carried out on the synthesized dye-NJ systems in THF solution
with increasing amounts of acid. Our previous studies have shown that
in the presence of 100 equivalents of acid, pz-NJs are completely
broken down. As expected, the fluorescence of the dyes is restored
close to the value of the free dye in the presence of 100 equiv of
acid (Figure S19).
Figure 4
Steady-state fluorescence
spectra after excitation at 350 nm of
free pyrene ligands (8.4 × 10–6, 6.0 ×
10–6 and 6.4 × 10–6 M, respectively)
and NJ-bound ligands (5.9 × 10–6, 8.4 ×
10–6 and 6.4 × 10–6 M, respectively)
in ACN for (A) L1, (B) L2 and (C) L3. Insets show the normalized fluorescence spectra of free
pyrene ligands and NJ-bound ligands.
Steady-state fluorescence
spectra after excitation at 350 nm of
free pyrene ligands (8.4 × 10–6, 6.0 ×
10–6 and 6.4 × 10–6 M, respectively)
and NJ-bound ligands (5.9 × 10–6, 8.4 ×
10–6 and 6.4 × 10–6 M, respectively)
in ACN for (A) L1, (B) L2 and (C) L3. Insets show the normalized fluorescence spectra of free
pyrene ligands and NJ-bound ligands.To understand the mechanism of fluorescence quenching in pyrene-bound
NJs, time-resolved fluorescence measurements were carried out using
time-correlated single photon counting. The free dyes and NJ-bound
dyes were excited with a 373 nm diode and fluorescence of pyrene was
monitored at 400 nm. Parts A, B, and C of Figure show the comparative decay traces for HL1, HL2, HL3 and the corresponding
NJs, respectively. The fluorescence decay of pyrene is faster when
bound to NJs than in the free form in solution. A significantly faster
decay was observed for L2 and L3 bound to
the NJs, compared to L1. Fluorescence lifetimes were
determined by fitting the decay traces to a multi-exponential decay
function and the obtained lifetime data are provided in Table . Two decay components were
obtained for HL1 in ACN with lifetimes of 2.1 ns (3.3%)
and 11.7 ns (96.7%). An average lifetime was determined using the
equation τavg = ∑aτ/∑a, which provides a value of
11.4 ns for HL1. For L1-NJ, the decay is
again fit to a double exponential function providing an average lifetime
of 10.9 ns. The decrease in fluorescence lifetime is marginal in the
case of L1-NJ, suggesting that the observed steady-state
quenching is mostly static in nature. In contrast, the fluorescence
decay of L2 was fit with two lifetime components of 3.2
ns (19.6%) and 14.4 ns (80.4%) and an average lifetime of 12.2 ns
was obtained. However, the decay of L2-NJ is much faster
than that of HL2 and triple exponential decay was needed
to fit the decay. An average lifetime of 4.4 ns is determined for L2-NJ indicating that the fluorescence quenching has contributions
from dynamic quenching. Similarly, a decreased average lifetime of
5.4 ns was obtained for L3-NJ when compared to HL3 (13.3 ns). The varying photoluminescence quenching observed
for the different pyrene derivatives bound to copper NJs is likely
related to the distance between fluorophore and NJ, as well as to
the orientation of the fluorophore on the NJs. Additionally, through-bond
vs. through-space fluorescence quenching needs to be considered in
these systems.
Figure 5
Fluorescence kinetic decay traces for the free dye and
NJ-bound
dye in ACN at 400 nm for (A) L1, (B) L2 and
(C) L3 after excitation at 370 nm.
Table 2
Fluorescence Lifetimes of the Synthesized
Pyrene Derivatives and the Corresponding NJs
Fluorescence kinetic decay traces for the free dye and
NJ-bound
dye in ACN at 400 nm for (A) L1, (B) L2 and
(C) L3 after excitation at 370 nm.A 6.3-fold steady-state fluorescence
quenching is observed for L1-NJ, which is much smaller
than the corresponding quenching
for L2-NJ (25-fold) and L3-NJ (19-fold).
Due to the structure of the tether, through-bond fluorescence quenching
is only possible in the case of L1-NJ. Surprisingly, L1-NJ shows the least fluorescence quenching among the fluorescent
NJ systems studied, despite the fact that the pyrene moiety is the
closest to the paramagnetic Cu2+ centers in L1-NJ. Time-resolved fluorescence measurements have shown little to
no decrease in lifetime for L1-NJ, while 2.7- and 2.4-fold
lifetime quenching is observed for L2-NJ and L3-NJ, respectively. The fact that the lifetime change is negligible
for L1-NJ indicates that most of the fluorescence quenching
in this system is static in nature, with increased inter-system crossing
as the pyrene is closer to the paramagnetic copper centers in the
NJ. Additional fluorescence lifetime quenching is observed for L2-NJ and L3-NJ indicating a contribution of
dynamic quenching. The dynamic quenching contribution is likely arising
from the fact that L2 and L3 possess flexible
aliphatic tethers that allow for a closer contact between the pyrene
chromophore and the NJ. Current time-resolved fluorescence measurements
with limited time resolution (∼1 ns) are unable to capture
faster deactivation pathways that are apparent in pyrene-bound NJs.
Therefore, ultrafast time-resolved measurements are needed on these
systems, which will be addressed in upcoming studies.
Conclusions
In summary, three novel pyrene-functionalized pyrazole ligands
(HL1, HL2, and HL3) as well
as the corresponding NJs containing these fluorescent ligands were
synthesized and characterized using NMR spectroscopy, mass spectrometry,
and photophysical techniques. Steady-state fluorescence measurements
indicate strong and varied fluorescence quenching for these ligands
when bound to NJs. With L1, where the pyrene fluorophore
is directly bound to the copper NJ, a 6.3-fold quenching was observed,
whereas with L2 and L3 the quenching is
25- and 19-fold, respectively. Time-resolved fluorescence measurements
have shown only static quenching for L1-NJ, while significant
contribution from dynamic quenching is observed for L2-NJ and L3-NJ. The additional dynamic quenching has
origins in the flexibility of L2 and L3 which
allows for the pyrene moiety to fold back onto the NJs. Because Cu2+ is the only metal ion that can be used for the preparation
of NJs, future studies will focus on the attachment of the fluorophore
using rigid, non-conjugated tethers, which will minimize fluorescence
quenching caused by the paramagnetic Cu2+ ions.
Experimental
Section
General
All reagents used were purchased from commercial
sources and were used as received, unless otherwise specified. Solvents
were also used as received, except in the synthesis of Pd(PPh3)2Cl2, for which THF was dried using
sodium/benzophenone, and in the transformation of THP-protected 4-(3-bromopropyl)pyrazole
to the corresponding alkyne, for which DMF was dried over 4 Å
molecular sieves. Standard Schlenk techniques were used for reactions
sensitive to air and/or moisture, and degassing of solvents was performed
using the freeze–pump–thaw method. Water was deionized
and solvents used for mass spectrometry were mass spectrometry-grade.1-Bromopyrene,[52] 1-azidopyrene,[53] Pd(PPh3)2Cl2,[54] (Bu4N)2[CO3{Cu(OH)(pz)}] (n = 27, 29–31; pz-NJs),[4] and a mixture
of heteroleptic NJs based on a 9:1 molar ratio of pyrazole/4-(pent-4-yn-1-yl)pyrazole
were synthesized according to literature procedures.[49] Synthesis of the THP-protected 4-(4-pentynyl)pyrazole (in
5 steps) was also conducted according to referenced procedures,[49] with additional details and adjustments explained
herein. In the final step going from the THP-protected 4-(3-bromopropyl)pyrazole
to the alkyne product, fresh sodium acetylide (NaC≡CH) slurry
was used and 2.65 equiv (of pure sodium acetylide, i.e., not the slurry
mixture) were used in the reaction instead of 1.5 equiv listed in
the original procedure. All reagents for this final reaction were
added under inert atmosphere via syringe. For column chromatography,
a ratio of 2.5:1 hexanes/ethyl acetate was used instead of the 2:1
ratio to improve separation and reduce band overlap between the alkyne
and the allyl side product within the column. The first fractions
of organic material to leave the column contain mostly the allyl impurity,
and latter fractions contain the desired alkyne with increasing purity.
The impure fractions are purified in a second column using the same
solvent mixture listed here to yield THP-protected 4-(4-pentynyl)pyrazole
(yield of crude product: 83.3%; yield of purified product: 45%).Mass spectrometry was performed using a Waters Synapt G1 HDMS instrument
with electrospray ionization (ESI). The settings used for mass spectrometry
were as follows: capillary voltage of 2.5 kV, sampling cone voltage
of 40 V, extraction cone voltage of 2.5 V, source temperature of 80
°C, desolvation temperature of 110 °C, cone N2 flow rate of 45 L/h, desolvation N2 flow rate of 470
L/h. Samples were infused at 5 μL/min. All samples analyzed
with the mass spectrometer were dissolved in ACN. 1H NMR
spectra were collected using a Jeol JNM-ECZS (400 MHz) spectrometer.Steady-state ultraviolet–visible (UV–vis) and fluorescence
spectra were collected using a Shimadzu UV-1650PC UV–visible
spectrophotometer and a Horiba Jobin Yvon FluoroMax-3, respectively.
All UV–vis measurements were obtained at 25 °C. Slit widths
of excitation and emission were both 1 nm unless otherwise specified.
Time-resolved fluorescence measurements were taken on an Edinburgh
Instruments F900 spectrofluorometer, equipped with an 800-B pulsed
diode laser as the excitation source emitting an excitation wavelength
of 373 nm. Time-resolved fluorescence measurements were analyzed with
the Edinburgh-Instruments analysis software utilizing either reconvolution
or tail-fits.
Synthesis of 1-(Tetrahydro-2H-pyran-2-yl)pyrazole-4-boronic
Acid Pinacol Ester
Pyrazole-4-boronic acid pinacol ester
(1.50 g, 7.73 mmol), ACN (20 mL), 3,4-dihydro-2H-pyran
(776 μL, 715 mg, 8.51 mmol), and trifluoroacetic acid (50.0
μL, 74.5 mg, 0.653 mmol) were combined in a 50 mL round bottom
flask and the solution was refluxed under stirring overnight. After
cooling to room temperature, the reaction mixture was quenched with
saturated NaHCO3 solution until pH ≈ 8 was reached.
The resulting mixture was extracted with dichloromethane (30 mL ×
3) and the combined organic layers were dried over anhydrous Na2SO4. After filtration, the solvent was removed
under reduced pressure yielding 1.90 g of an orange oil that solidified
upon standing (yield: 89%). 1H NMR (400 MHz, CDCl3): δ 7.91 (s, 1H, 5-H-pz), 7.80 (s, 1H, 3-H-pz), 5.38 (dd, 1H, CH-THP, J = 9 Hz, 3 Hz), 4.02 (d, 1H, CH2O-THP, J = 10 Hz), 3.67 (td, 1H, CH2O-THP, J = 11 Hz, 3 Hz), 1.92–2.20 (m, 3H,
CH2-THP), 1.52–1.77 (m, 3H, CH2-THP), 1.28 (s, 12H, CH3) ppm. 13C NMR (101 MHz, CDCl3): δ 145.5, 134.8,
87.4, 67.8, 30.6, 25.0, 24.9, 24.8, 22.4 ppm. HRMS (ESI-TOF) m/z: [M + Na]+ calcd for C14H23BN2O3Na, 300.1736; found,
300.1754.
Synthesis of 4-(Pyren-1-yl)pyrazole (HL1)
In a round-bottom Schlenk flask fitted with a septum, 1-(tetrahydro-2H-pyran-2-yl)pyrazole-4-boronic acid pinacol ester (1.53
g, 5.5 mmol) and 1-bromopyrene (1.95 g, 6.95 mmol) were added. The
flask was purged with N2(g) and a degassed mixture of dioxane
and water (5:1, 15 mL) was added via syringe. K2CO3 (2.93 g, 21.2 mmol) was added, followed by Pd(PPh3)4 (0.460 g, 0.40 mmol). The walls of the flask were rinsed
with the dioxane solution, and a condenser was fitted. The reaction
mixture was refluxed under inert atmosphere overnight. Water was added
to the red solution, and the product was extracted with ethyl acetate
(80 mL × 2). The combined organics were washed with brine (40
mL) and dried over Na2SO4. After filtration,
the solvent was removed under reduced pressure.The crude product
was dissolved in a 1:50 mixture of dichloromethane and ethanol (100
mL). Concentrated sulfuric acid (5.5 mL) was added dropwise and the
reaction was vigorously stirred for 24 h. The reaction was quenched
with NaHCO3 to a pH of ∼8. The product was extracted
with chloroform (80 mL × 2), and the organic phase was washed
with water and brine followed by drying over Na2SO4, filtration and removal of solvent under reduced pressure.
The crude product (2.63 g) was purified by flash chromatography on
silica gel using a 2:1 mixture of ethyl acetate and hexanes (Rf = 0.36) to yield 702 mg of a yellow solid
(yield: 48%). Using a 1:1 molar ratio of the pinacol ester starting
material and 1-bromopyrene produces a 50% overall yield.[49]1H NMR (400 MHz, DMSO-d6): δ 8.44 (d, 1H), 8.26–8.31 (m, 4H), 8.16–8.20
(m, 3H), 7.90–8.10 (m, 3H) ppm. 13C NMR (101 MHz,
DMSO-d6): δ 139.7, 131.6, 131.1,
130.0, 129.4, 128.9, 128.2, 128.1, 128.0, 128.0, 127.5, 126.9, 125.7,
125.3, 124.9, 124.7, 120.2 ppm. HRMS (ESI-TOF) m/z: [M – H]- calcd for C19H11N2, 267.0922; found, 267.0952.
Synthesis of
4-(5-(Pyren-1-yl)pent-4-yn-1-yl)pyrazole (HL2)
The THP-protected pentynyl-pyrazole (320 mg,
1.47 mmol) was added to a 50 mL Schlenk flask. 1-Bromopyrene (414
mg, 1.47 mmol) was added, followed by PdCl2(PPh3)2 (110 mg, 0.16 mmol). Triethylamine (12 mL) was added
to the flask and the mixture was purged with nitrogen while stirring.
CuI (3 mg, 0.016 mmol) was added to the flask and stirred at 65 °C
overnight using an oil bath. The deep red/brown mixture was cooled
to room temperature and filtered. The flask was rinsed with EtOAc,
which was filtered and combined with the previous filtrate. Then,
the solvent was removed under reduced pressure yielding 669 mg of
crude product, which was dissolved with minimal methanol. p-Toluene sulfonic acid monohydrate (608 mg) was added to
the solution until a pH of 3 and was stirred for two days. The mixture
was quenched with saturated NaHCO3 solution to a pH of
∼8, then extracted with chloroform (100 mL × 3). The combined
organics were dried over Na2SO4 and the solvent
was removed under reduced pressure. The residue was dry loaded onto
a silica column and purified with flash chromatography (3:2 EtOAc/hexanes)
to yield 115 mg of an orange oil. A second column was performed on
impure fractions using 49:1 CHCl3/MeOH to yield an additional
30 mg of HL2 (overall yield: 30%). 1H NMR
(400 MHz, CDCl3): δ 8.56 (d, 1H), 7.99–8.21
(m, 8H), 7.52 (s, 2H), 2.83 (t, 2H, J = 8 Hz), 2.69
(t, 2H, 8 Hz), 2.04 (m, 2H, 7 Hz) ppm. 13C NMR (101 MHz,
CDCl3): δ 133.0, 131.9, 131.4, 131.2, 130.8, 129.7,
128.2, 127.9, 127.3, 126.2, 125.7, 125.5, 124.6, 124.5, 120.3, 118.8,
95.7, 80.3, 30.2, 23.4, 19.4 ppm.
Synthesis of 4-(3-(Pyrazol-4-yl)propyl)-1-(pyren-1-yl)-1,2,3-triazole
(HL3)
4-(4-Pentyn-1-yl)-1-(tetrahydro-2H-pyran-2-yl)pyrazole (270 mg, 1.24 mmol) and 1-azidopyrene
(303 mg, 1.25 mmol) were dissolved in degassed THF (15 mL) in an oven-dried
2-neck Schlenk round-bottom flask fitted with a septum. The flask
was purged with N2(g). A solution of CuSO4·5H2O (463 mg, 1.86 mmol) in H2O (10 mL) was transferred
to the reaction vessel via syringe. A fresh solution of sodium ascorbate
in H2O (15 mL), prepared from ascorbic acid (1.31 g, 7.44
mmol) and NaHCO3 (625 mg, 7.44 mmol), was added dropwise.
The walls of the flask were rinsed with THF and the reaction mixture
was stirred at room temperature under inert atmosphere for three days.
The deep red/brown solution was quenched to neutral pH with NH4OH (30% wt) solution. The mixture was extracted with chloroform
(50 mL × 4), and the combined organics were washed with H2O (60 mL × 2) and brine (120 mL). The organic layer was
dried over MgSO4, then it was filtered and the solvent
was removed by evaporation. The residue was dissolved in EtOH (50
mL) and concentrated sulfuric acid was added dropwise via pipette
until the solution had a pH of 3. This reaction mixture was stirred
overnight, then was quenched with saturated NaHCO3 solution
to a pH of 8. The mixture was extracted with chloroform (60 mL ×
3), and the combined organics were washed with H2O (120
mL × 2) and brine (120 mL × 2). The organic layer was dried
over Na2SO4, filtered, and concentrated. The
resulting red/brown solid was dissolved in a minimal amount of chloroform,
and excess diethyl ether was added while mixing to form a brown precipitate.
The precipitate was filtered and washed with diethyl ether. Residual
solvent was removed from the precipitate under reduced pressure to
yield 241 mg of HL3. Evaporating the filtrate followed
by dissolving the residue in chloroform and precipitating with ether
yielded an additional 16 mg of HL3 (overall yield: 55%). 1H NMR (400 MHz, DMSO-d6): δ
8.57 (s, 1H, triazole-H), 8.49–8.18 (m, 8H,
pyrene-H), 7.80 (d, 1H, pyrene-H, J = 9 Hz), 7.51 (br, 2H, 3,5-H-pz), 2.85 (t, 2H, C pz-CH2CH2, J = 7 Hz), 2.60 (t, 2H, CH2CH2C, J = 7 Hz), 2.02 (m, 2H,
CH2CH2CH2) ppm. 13C NMR (101 MHz, DMSO-d6): δ
147.8, 132.1, 131.3, 131.2, 130.7, 130.1, 129.3, 127.7, 127.1, 126.7,
125.9, 125.7, 125.7, 124.6, 124.4, 123.9, 121.7, 119.8, 31.1, 25.2,
23.8 ppm. HRMS (ESI-TOF) m/z: [M
+ Na]+ calcd for C24H19N5Na, 400.1538; found, 400.1533.
Synthesis of Fluorescent
NJs
All NJs in this study
were synthesized by standard procedures[4] with details mentioned here. The fluorescent ligand (0.05 mmol)
was combined with pyrazole (0.95 mmol) in a 1:19 ratio, respectively,
to total 1 mmol in a round bottom flask. Cu(NO3)3·2.5H2O (1 mmol) was added, followed by THF (10 mL).
NaOH pellets (2.13 mmol) were ground with a mortar and pestle, then
added to the THF solution. Na2CO3·H2O (1 mmol) was added to the dissolved mixture, capped, and
stirred at room temperature for three days. The blue solution was
then filtered, and the solvent allowed to evaporate. The residue was
redissolved in THF and filtered into a clean beaker to evaporate once
more, yielding a blue solid.The blue NJ solids were dissolved
in minimal ACN and stirred for 1 h. This solution was added dropwise
to isopropyl ether (threefold excess) and stirred for an additional
30 min. After filtration, a dark-colored residue remained on the filter
medium. The solvent was removed under reduced pressure, yielding clean
NJs without any free fluorescent dyes (verified with fluorescence
spectroscopy).Click coupling reactions were conducted in degassed
solvent and
were stirred for 5 days under N2. 0.1155 g NJ and 1-azidopyrene
(0.0359 g) were dissolved in either THF (15 mL), ACN (10 mL), or a
mixture of THF/ACN (1:1 v/v, 20 mL). A stock solution of CuI was prepared
with 0.0791 g of CuI dissolved in 10 mL of ACN. 710 μL of this
solution was added to the reaction mixture and was stirred in the
dark.
Titration of 1-Bromopyrene with (Bu4N)2[CO3{Cu(OH)(pz)}] (n = 27, 29–31; pz-NJs)
Solutions of 1-bromopyrene
(3.20 μM) and pz-NJs (4.11 μM) were prepared in ACN and
were both measured to have an absorbance of 0.12 at 345 nm. Before
any titrant was added, the absorbance and emission spectra of the
1-bromopyrene solution (3 mL) was collected as a baseline. 50 μL
of the NJ solution was then added to the cuvette containing the analyte,
and the absorbance and emission spectra were collected again. This
process was repeated in 50 μL additions until a total of 1 mL
of NJ solution was added to the cuvette (1 cm path length). The emission
spectra were obtained by exciting the solution at 345 nm and monitoring
the fluorescence from 360 to 550 nm (using a 5 nm slit width setting).
Titration of L1-NJ, L2-NJ and L3-NJ with Acid
Nitric acid was selected as a titrant
because the nitrate ion is known not to interfere with NJs even at
high concentrations. Two separate solutions were prepared using a
serial dilution method to yield 0.038 M and 0.001 M HNO3 in THF. A 14 μM L1-NJ solution was prepared in
THF (10 mL). The absorbance and emission spectra of the L1-NJ solution was collected. Two equivalents of HNO3 (i.e.,
279 μL of 0.001 M nitric acid solution) were then added to the L1-NJ solution, and the absorbance and emission spectra were
collected. This step was repeated after adding additional amounts
of acid. Thus, fluorescence spectra were collected for L1-NJs with 0, 2, 10, 20, and 100 equiv of HNO3, indicating
an increase in fluorescence intensity with increasing acid equivalents.
Each solution was excited at 350 nm and the fluorescence was monitored
from 365 to 550 nm (slit widths 5 and 2.5 nm for excitation and emission,
respectively). Similar procedures were employed using L2-NJ (8.8 μM in THF) and L3-NJ (2.3 μM in
THF).