A Highly Luminescent Nitrogen-Doped Nanographene as an Acid- and Metal-Sensitive Fluorophore for Optical Imaging.

Dibenzo[hi,st]ovalene (DBOV) has excellent photophysical properties, including strong fluorescence and high ambient stability. Moreover, the optical blinking properties of DBOV have enabled optical super-resolution single-molecule localization microscopy with an imaging resolution beyond the diffraction limit. Various organic and inorganic fluorescent probes have been developed for super-resolution imaging, but those sensitive to pH and/or metal ions have remained elusive. Here, we report a diaza-derivative of DBOV (N-DBOV), synthesized in eight steps with a total yield of 15%. Nitrogen (N)-bearing zigzag edges were formed through oxidative cyclization of amino groups in the last step. UV-vis and fluorescence spectroscopy of N-DBOV revealed its promising optical properties comparable to those of the parent DBOV, while cyclic voltammetry and density functional theory calculations highlighted its lower orbital energy levels and potential n-type semiconductor character. Notably, in contrast to that of the parent DBOV, the strong luminescence of N-DBOV is dependent on pH and the presence of heavy metal ions, indicating the potential of N-DBOV in sensing applications. N-DBOV also exhibited pH-responsive blinking, which enables pH-sensitive super-resolution imaging. Therefore, N-DBOV appears to be a highly promising candidate for fluorescence sensing in biology and environmental analytics.

Introduction

The ability to locally, and with high precision, determine pH and/or the presence of specific metal ions using fluorescent molecules is important for several disciplines, including biology[1−4] and environmental monitoring.[5−7] Detection of transition metal ions is crucial to the diagnosis and/or prevention of diseases caused by dysregulation of metal-ion homeostasis, such as anemia and Alzheimer’s disease.[4] In biology, protons play a critical role in living cells to support various biological activities.[8] The currently available pH- and/or metal ion-sensitive fluorophores consist of two classes: organic dyes[9] and nanomaterial-based probes,[10] e.g., carbon dots[11,12] and semiconductor quantum dots,[13,14] which have been intensively investigated in the past decade. Organic dyes, such as rhodamines and cyanine derivatives, can detect systems with high specificity and brightness.[2,9] On the other hand, carbon dots and quantum dots can serve as low-cost probes with high chemical stability.[15] However, the limited photostability, resulting in fast photobleaching, remains a common bottleneck for most existing probes.[16] Different approaches, such as excitation light dose engineering[17] and use of anti-fading agents,[16] have been proposed to suppress the photobleaching, but such methods still typically increase the complexity of detection and narrow the range of applications.

On the other hand, pH-sensitive fluorescence probes, especially for optical super-resolution nanoscale imaging/detection beyond the diffraction limit of conventional light microscopy, remain rare.[2] Optical super-resolution microscopy includes two groups of methods: stimulated emission depletion (STED) microscopy[18] and single-molecule localization microscopy (SMLM).[19]

For STED microscopy, the fluorophores need to exhibit a significant amount of emission at the depletion wavelength of the used fluorophore, as this determines the efficiency of stimulated emission. Meanwhile, high brightness and photostability under the given imaging conditions are also prerequisites. Currently, only super-resolution pH indicator molecules based on the two-fluorophore design have been used as pH probes in STED microscopy, with a limited dynamic pH detection range of 5–7.[2] For SMLM, photoblinking fluorophores are needed,[20] and no pH-sensitive probe suitable for SMLM imaging has been reported, to the best of our knowledge.

Similar challenges exist for metal-ion sensing: most of the existing fluorophores are less suited for probing applications, including bioimaging, due to chemical or photophysical limitations.[21−23] In particular, to avoid possible photoinduced biosample damage, excitation light in the longer visible and near-infrared wavelength is preferred.[24] However, many reported metal-sensing dyes need higher photon energy for excitation, such as blue or even UV light, which is out of the biowindow.[24−27]

Clearly, new fluorescence probes with enhanced photostability and a wider dynamic range of pH detection and metal-ion probing, especially suitable for super-resolution microscopy, are in high demand.

Nanographenes, nanoscale polycyclic aromatic hydrocarbons (PAHs), have enormous promise because of their unique optical, electronic, and magnetic properties and potential applications in photonics, optoelectronics, and optical imaging.[28−34] Among the various reported nanographenes,[35−40] those with zigzag edges provide a particularly promising platform to explore electronic features such as narrow energy gaps and an open-shell biradical character.[41−44] However, nanographenes with zigzag edges are often unstable under ambient conditions.[45,46] Recently, Wu and co-workers reported a series of nanographenes with four zigzag edges and their integration into laser devices.[47] We recently synthesized dibenzo[hi,st]ovalene (DBOV) derivatives with both zigzag and armchair edges, which exhibited high stability and strong red luminescence with fluorescence quantum yields of up to 97%.[48−54] DBOV also displayed exceptional photophysical characteristics, such as intrinsic blinking in very different environments, superior fluorescence recovery, and stability over several months.[55] These features make DBOV a unique fluorophore for optical super-resolution nanoscale imaging,[55] although its hydrocarbon structure prohibits its use in sensing applications. Nanographene with some of its carbon atoms replaced by nitrogen atoms would be an excellent potential candidate for pH and metal-ion sensing, given the possibility of protonation of the nitrogen atom and its metal-ion chelating potential. Both are expected to modify the electronic structure and thereby the fluorescence properties of nanographene.[56,57] According to the literature, the most probable fluorescence quenching mechanism of fluorophores with a nitrogen-incorporated structure is through protonation of the nitrogen atom and, for metal ions, photoinduced electron transfer (PET)[58] upon coordination directly to metal ions. For a nitrogen-substituted nanographene, one may expect high proton/ion sensitivity owing to the nitrogen atom being part of the fluorescent aromatic core.

Nitrogen (N)-incorporation into PAHs has been extensively studied to tune their orbital energy levels, redox properties, and chemical reactivity.[59−67] For example, aza derivatives of perylene,[59,60] pyrene,[61] coronene,[62,63] and dibenzoperylene[64] have been reported, demonstrating their n-type semiconductor character, acid-sensitive optical responses, and coordination to metal ions. N-containing heteroacenes with N-bearing zigzag edges have attracted considerable attention as active components of organic electronics, with repeated attempts to achieve higher N-heteroacenes.[65−67] N incorporation into large PAHs, namely, nanographenes, has also been explored, thus providing models of N-doped graphene with increasing relevance to fundamental research and applications.[56,68−74] For example, an electron-deficient N-containing hexa-peri-hexabenzocoronene (HBC) with fused pyridine rings,[56] electron-rich hexapyrrolohexaazacoronenes,[73] and an antiaromatic pyrazine-embedding HBC[74] were reported, although the latter could be obtained only on a metal surface under ultra-high-vacuum conditions. However, nitrogen-doped nanographenes, especially those with N-bearing zigzag edges, are rare.[67]

In this work, we introduce nitrogen atoms into the zigzag edges of DBOV to establish 6,14-diazadibenzo[hi,st]ovalene (N-DBOV 10) as a new N-doped nanographene. N-DBOV 10 presents unique opportunities for pH- and metal-ion sensing by fluorescence microscopy. N-DBOV 10 could be synthesized in eight steps with a total yield of 15% from commercially available starting material 1. N-DBOV 10 displayed high photostability and lowered orbital energy levels, as revealed by cyclic voltammetry and density functional theory (DFT) calculations. Furthermore, spectroscopic characterizations demonstrate the pH- and metal-ion-sensitive behavior of N-DBOV 10, showing quick quenching of the strong luminescence upon addition of acid or metal ions, such as Cu2+ and Fe2+. pH-dependent fluorescence blinking was also observed for N-DBOV 10, indicating potential applications in nanoscale pH measurements in biological, environmental, and material research.

Results and Discussion

Synthesis of N-DBOV 10

The synthesis of N-DBOV 10 was carried out as shown in Scheme . The key intermediate 9, with two amino groups, was prepared by adapting our previous procedure for another derivative with two formyl groups.[48] 3-Bromo-4-triisopropylsilyl (TIPS)-ethynyl-tert-butylbenzene (2) was obtained though the Sonogashira reaction of 3-bromo-4-iodo-tert-butylbenzene (1) and TIPS-acetylene in 93% yield. Bromide 2 was lithiated with n-butyllithium (n-BuLi) and then reacted with triisopropyl borate to give 5-tert-butyl-2-(TIPS-ethynyl)phenylboronic acid (3) in 78% yield, which was subsequently subjected to Suzuki coupling with naphthyl triflate 4 to afford 7-{5-tert-butyl-2-(TIPS-ethynyl)phenyl}-2-naphthylamine (5) in 83% yield. After deprotection of 5 with tetra-n-butylammonium fluoride (TBAF) to provide 6 in 94% yield, a Cu-mediated Glaser coupling of 6 provided diaryldiacetylene 7 in 87% yield. Subsequently, iodination-benzannulation[75,76] of 7 by treatment with ICl gave diiodobichrysenyl 8 in 73% yield. Photochemical cyclodehydroiodination[77] of 8 in the presence of triethyl amine (TEA) provided fused product 9, which was directly used for the next step. For the formation of the N-bearing zigzag edges, the use of the Cadogan reaction conditions[78] was initially considered. When the oxidation of the amino groups of 9 to the nitro groups was attempted by treatment with tert-butyl hydroperoxide (TBHP) as the oxidant and KI as the catalyst,[79] we found that N-DBOV 10 was directly formed instead in 42% yield over two steps. We assume that the amino group of 9 is activated by the tBuO radical, which is generated through the decomposition of TBHP mediated by KI,[80,81] followed by intramolecular cyclization instead of further oxidation to the nitro group (see Scheme S1 for a possible mechanism). To the best of our knowledge, this is the first example of the direct oxidative cyclization of the amino group to form an N-incorporated PAH,[70,82,83] which can potentially be useful for the synthesis of a wider variety of aza-PAHs.

Scheme 1

Synthesis of N-DBOV 10

Reagents and conditions: (i) Pd(PPh3)2Cl2 (0.02 equiv), CuI (0.04 equiv), THF/TEA (1:1), RT, 12 h; (ii) n-BuLi (1.2 equiv), THF, −78 °C, 2 h, B(OiPr)3 (2.0 equiv), RT, overnight; (iii) Pd(PPh3)4 (0.05 equiv), K2CO3 (6.0 equiv), toluene/EtOH/H2O (4:1:1), 80 °C, overnight; (iv) TBAF (1.2 equiv), THF, RT, 3 h; (v) Cu(OAc)2 (1.0 equiv), MeOH/pyridine (1:1), 80 °C, overnight; (vi) ICl (2.1 equiv), DCM, −78 °C, 2 h; (vii) TEA (excess), toluene, hυ, 2 h; (viii) TBHP (2.5 equiv), KI (0.1 equiv), CH3CN/H2O, 60 °C. THF: tetrahydrofuran, TEA: trimethylamine, DCM: dichloromethane, TBHP: tert-butyl hydroperoxide.

Electron ionization high-resolution mass spectrometry (EI-HRMS) analysis of N-DBOV 10 revealed an intense signal at m/z = 587.2481, in agreement with the calculated mass of m/z = 587.2482 ([M + H]+). Limited solubility and strong intermolecular interactions of N-DBOV 10 hindered its NMR characterizations in its neutral form, while its 1H NMR spectrum could be recorded in trifluoroacetic acid (TFA)-d at 298 K as a dideuterated form, N-DBOV-2D+ (Figure S12), and all the proton resonances were assigned on the basis of their 1H,1H-correlation spectroscopy (COSY) and 1H,1H-nuclear Overhauser effect spectroscopy (NOESY) spectra (see the SI, Figures S1–S22). To determine the effect of N incorporation on the optical and electronic properties of the DBOV core, excluding the possible effects of alkyl or aryl substituents on the zigzag edges of previously reported DBOVs, a new DBOV derivative 11 was designed as a reference compound with bare zigzag edges and two tBu groups in the same positions as those in 10 (Figure ). The synthesis of 11 was carried out by adapting our previous procedure reported for other DBOV derivatives (see the SI for details).[48]

Figure 1

Chemical structures of N-DBOV 10 and DBOV 11. The numbers inside the six-membered rings indicate NICS(1) values.

Optical and Electronic Properties

The UV–vis absorption spectra of N-DBOV 10 and DBOV 11 in tetrahydrofuran (THF) were very similar, exhibiting absorption maxima at 580 and 586 nm, respectively, with a vibronic progression at shorter wavelengths (Figure ). These absorption bands were assigned to the HOMO–LUMO transitions based on time-dependent density functional theory (TD-DFT) calculations at the B3LYP/6-31G(d) level of theory (Figure S23 and Table ).

Figure 2

UV–vis absorption and photoluminescence (PL) spectra of 10–6 M solutions of N-DBOV 10 (red) and DBOV 11 (black) in THF measured at room temperature.

Table 1

Optical and Electrochemical Properties of N-DBOV 10 and DBOV 11

compound	λmax (nm)	λem (nm)	ϕα	τ (ns)	Eg(opt) (eV)a	Eg(cal) (eV)b	HOMO(cal) (eV)b	LUMO(cal) (eV)b	HOMO(CV) (eV)c
N-DBOV 10	580	591	0.76	6.0	2.07	2.20	–4.99	–2.79	–4.83
DBOV 11	586	594	0.80	7.5	2.05	2.13	–4.48	–2.35	–4.75

Optical gaps were estimated based on the wavelengths at which the normalized absorption and fluorescence spectra cross each other.

DFT calculations were performed at the B3LYP/6-31G(d) level of theory with the Gaussian 16 calculation package.[85]

The HOMO energy levels were estimated by utilizing the onset of the first oxidation potential of CV calibrated with Fc/Fc+.

Similar to previously reported DBOV derivatives, N-DBOV 10 demonstrated strong red emission.[48,49] Fluorescence spectra of N-DBOV 10 and DBOV 11 showed maxima at 588 and 594 nm, respectively, with Stokes shifts of 235 and 230 cm–1, respectively (Figure ). The UV–vis and fluorescence spectra of 10 and 11 displayed more significant broadening compared with a previously reported DBOV derivative with two mesityl groups (Figure S24), which could be ascribed to the higher aggregation tendency of 10 and 11. Nevertheless, shifts of their absorption and emission maxima were negligible in the concentration range of 10–4 to 10–7 M. The optical gaps of 10 and 11 were estimated to be 2.12 and 2.10 eV, respectively, from the wavelengths at which their normalized absorption and fluorescence spectra cross each other (Table ). The fluorescence quantum yields of 10 and 11 were assessed using Nile blue A perchlorate as a standard to be 76% and 80%, respectively (Table ). The absorption and fluorescence spectra of 10 displayed no significant variations (peak shifts below 8 nm) in different solvents with varying polarities, including toluene, THF, and dimethylformamide (Figure S25). These results indicated that N incorporation on the zigzag edges had a negligible effect on the static optical properties of the DBOV core. On the other hand, the fluorescence lifetime of N-DBOV 10 was determined to be 6.0 ns, which was slightly shorter than the value of 7.5 ns measured for DBOV 11 (Figure S26).

The electrochemical properties of N-DBOV 10 and DBOV 11 were characterized by cyclic voltammetry (CV) in anhydrous THF solutions at room temperature (Figure S27). In the CV curves of 10 and 11, the onset of the first oxidation potentials occurred at 0.03 and −0.05 V, respectively, against Fc/Fc+, corresponding to HOMO energy levels of −4.83 and −4.75 eV, respectively, according to the equation HOMO = −(4.8 + Eoxonset) (Table ). This result indicated that N incorporation lowered the orbital energy level without significantly affecting the static optical properties discussed above, in line with previous reports for other N-bearing PAHs.[84]

DFT calculations also revealed that N-DBOV 10 possesses lower-lying HOMO and LUMO energy levels (−4.99 and −2.79 eV) than DBOV 11 (−4.48 and −2.35 eV) but similar HOMO–LUMO energy gaps of 2.20 and 2.13 eV, respectively (Figure and Table ).

Figure 3

HOMOs and LUMOs of N-DBOV 10 and DBOV 11 calculated by DFT at the B3LYP/6-31G(d) level.

To examine the influence of N incorporation on the aromaticity of the DBOV core, nucleus-independent chemical shift (NICS) calculations were performed for N-DBOV 10 and DBOV 11 at the GIAO-B3LYP/6-31G(d) level of theory (Figure ).[86,87] The results for N-DBOV 10 and DBOV 11 were similar, indicating strong aromaticity in rings A, D, and F with negative NICS(1) values ranging from −31.15 to −21.42. The anisotropies of the induced current density (ACID)[88] plots of N-DBOV 10 and DBOV 11 were almost identical, displaying a clockwise (diatropic) ring current at an isosurface value of 0.05 (Figure S28).[51] The NICS(1) and ACID results indicate that N incorporation in the zigzag edges does not significantly affect the DBOV core aromaticity.

Fluorescence Properties of N-DBOV

Fluorescence Stability

To examine the suitability of N-DBOV 10 for fluorescence imaging, we first compared the photostability of N-DBOV 10 with that of the commonly used organic dyes Alexa 647 and DBOV 11 deposited on glass coverslips (Figure ).

Figure 4

Photobleaching properties of N-DBOV 10 (red), DBOV 11 (blue), and Alexa 647 (black) as a function of the imaging time.

To our delight, under the same continuous 532 nm laser excitation conditions in air, N-DBOV 10 maintained 74% of its fluorescence intensity after irradiation for up to 450 s, while Alexa 647 was quickly photobleached within 45 s (see the SI and Figure S29 for more details). DBOV 11 retained ∼66% of its fluorescence intensity for 450 s. Other dyes typically require antifading agents[21,36] to improve their photostability. The high stability of N-DBOV allows its use in imaging applications with few constraints on its environment.

Protonation of N-DBOV 10

The acid sensitivity of N-DBOV 10 was investigated by monitoring the changes in UV–vis absorption while adding TFA. During the addition of up to 1.0 equiv of TFA to a solution of N-DBOV 10 in DCM, new broad absorption bands centered at 507 and 630 nm replaced the original peaks at 541 and 584 nm, resulting in isosbestic points at ∼526 and 609 nm (Figure a). The disappearance of the original N-DBOV absorption upon the addition of 1.0 equiv of TFA indicates complete conversion to N-DBOV-H+. Further addition of TFA up to 2.0 equiv increased the absorbance, with the appearance of well-resolved peaks at 498, 528, 612, and 667 nm (Figure b). An excess (5.0 equiv) of TFA did not change the spectrum, indicating that the formation of N-DBOV-2H+ was complete with 2.0 equiv of TFA. The acquired absorption spectra of N-DBOV-2H+ were consistent with those obtained from TD-DFT calculations (Figure S30). Protonation of N-DBOV 10 also strongly affects its fluorescent response, leading to the very efficient fluorescence quenching. The fluorescence of N-DBOV 10 could be largely quenched intensity, which was not observed for DBOV 11 by 0.5 equiv of TFA, while DBOV 11 did not exhibit any quenching behavior (Figure c and d). Protonation of N-DBOV 10 with HCl also significantly decreased the fluorescence of 11 (see Figures S31 and S32). The fluorescence of N-DBOV 10 could be fully recovered by subsequently adding triethylamine (Figure S33), indicating the proton-sensing ability of N-DBOV 10. Based on the TD-DFT calculation, the fluorescence quenching of N-DBOV 10 under acidic conditions is attributed to a decrease in the radiative decay rate (Table S2).

Figure 5

(a, b) Changes in the UV–vis absorption spectrum upon titration of N-DBOV 10 (2 × 10–5 M in DCM) with TFA, monitoring the protonation of (a) N-DBOV 10 to N-DBOV-H+ and (b) N-DBOV-H+ to N-DBOV-2H+. The arrows indicate the changes in the intensity of each peak. (c, d) Changes in the fluorescence spectra of (c) N-DBOV 10 and (d) DBOV 11 in DCM solution (2 × 10–5 M in DCM) upon successive addition of TFA, recorded at room temperature.

Fluorescence Properties at the Single-Molecule Level

The pH-dependent blinking properties of N-DBOV 10 and DBOV 11 were further analyzed at the single-molecule level (Figure and Figure S34; see the SI for details). The number of active fluorophores and their numbers of emitted photons were determined as a function of pH. For these measurements, N-DBOV 10 molecules were first immobilized on a polystyrene-coated coverslip and then exposed to aqueous solutions with different pH values. The single-molecule fluorescence data are fully consistent with the ensemble measurements shown in Figure . Such single-molecule pH-dependent fluorescence could be used for super-resolution pH measurements.

Figure 6

Results of single-molecule fluorescence measurements of (a) N-DBOV 10 and (b) DBOV 11 exposed to aqueous solutions with different pH values. Note the reversible pH dependence of the number of active emitters (red line) in only (a), while the fluorescence intensity for each active emitter (number of photons, black line) is retained.

As presented in Figure a, over 87% of the excited N-DBOV 10 molecules were quenched when the pH was decreased from 7 to 1, while the remaining molecules showed almost constant brightness. Meanwhile, DBOV 11 showed no significant pH-dependent fluorescence changes (Figure b).

After neutralizing the pH 1 solution by adding the same volume of an aqueous NaOH solution (0.1 M), the fluorescence of the quenched N-DBOV 10 molecules recovered, in agreement with the ensemble experiments. Therefore, N-DBOV 10 is stable under acidic conditions and sensitive to pH, making it attractive as a pH sensor with a low detection limit.

Optical Imaging Applications

3D Confocal Imaging

To further assess the potential imaging applications of N-DBOV 10, a 3D confocal imaging experiment was carried out. As shown in Figure , gridded structures in a glass substrate with a width and depth of 5 μm each (Ibidi, gridded glass coverslips, Grid-50) were imaged after deposition of N-DBOV 10 as the fluorescence probe. The sample was first imaged by conventional bright-field microscopy and then with confocal microscopy at each z-position. Along the z-direction, a series of 2D images on the xy plane were acquired with a step size of 0.13 μm.

Figure 7

3D bright-field and confocal microscopy images of gridded structures in a glass substrate with N-DBOV 10. Reconstructions of the (a) bright-field 3D image and (b) confocal fluorescence 3D image. (c) Bright-field image and (d) confocal fluorescence image, both at an imaging depth of 11.83 μm relative to the surface of the glass substrate.

Finally, 3D volumes were reconstructed with the image processing software ImageJ. From our 3D confocal microscopy imaging (Figure b and d), micro- and nanostructures with a depth up to 17 μm could be imaged, which are difficult to visualize with other techniques, such as bright-field microscopy (Figure a and c). N-DBOV 10 demonstrated excellent photostability during the whole process. All images were reconstructed from two averaged line scans, and two full 3D images were recorded sequentially, taking 16 min in total. The two 3D images showed that the fluorescence intensity was very stable, and no photobleaching was observed (see the SI, Figures S35–S36, Table S3, and Supporting Videos 1–4 for more details). We note here that realistic 3D confocal imaging can be achieved using a much shorter exposure time. The longer exposure time used here mainly served to demonstrate the photostability of N-DBOV 10.

Optical Super-Resolution SMLM Imaging

For optical super-resolution SMLM imaging, blinking fluorescence with high photon numbers (detected photons per switching event) and low on–off duty cycle (fraction of time a molecule resides in its fluorescent state) are preferred.[23] High photon numbers provide high imaging resolution, while a low on–off duty cycle could improve both the imaging accuracy and labeling density by decreasing the probability of two fluorophores fluorescing simultaneously within the diffraction-limited imaging area.[23] However, the current gold-standard SMLM fluorophores, i.e., organic dyes in blinking buffer, typically degrade within hours.[89,90] These boundary conditions increase the imaging complexity and limit the imaging environment and imaging time. Similar to its parent DBOV,[54] the nanographenes presented here exhibited intrinsic blinking properties, independent of environment.

Investigation of N-DBOV 10 by single-molecule fluorescence analysis[61] demonstrated excellent blinking features, including high photon numbers of >6000 and low on–off-duty cycles of ∼10–3 with a blinking time of approximately 100 ms, in different environments, including in air, embedded in a polystyrene (PS) film, and in water (see the SI and Figure S37 for details about sample preparation and measurements). These results indicated the excellent suitability of N-DBOV 10 for optical super-resolution SMLM imaging. As a proof of concept, we performed an SMLM experiment using N-DBOV 10 to image nanoscale crevices in a glass substrate. Figure shows a direct comparison of the imaging results from conventional wide-field (WF) microscopy (Figure a) and the SMLM method (Figure b).

Figure 8

Optical fluorescence imaging of nanometer-sized crevices in a glass substrate with N-DBOV 10. (a) Wide-field image and (b) super-resolution SMLM image. Intensity profiles of (c) the wide-field image and (d) the super-resolution SMLM image indicated using the red line shown in the images of (a) and (b), respectively.

In the SMLM imaging, N-DBOV 10 molecules could be localized with an average localization precision of 21 nm. Compared to that of the WF image, the resolution of the SMLM image was significantly enhanced, with the SMLM method yielding an ∼6-fold reduction in the measured crevice width (Figure c and d). We note here that unlike other fluorophores commonly used for the SMLM method, which always require blinking buffer,[23] N-DBOV 10 enabled SMLM imaging in air without blinking buffer (see the SI for more details about the sample preparation and SMLM imaging analysis).

Metal-Ion Sensitivity

To investigate the ion-sensing capability of N-DBOV 10, its fluorescence response to different metal ions was examined. To this end, 9 × 10–4 M Cu2+, Fe2+, and Mg2+ solutions were prepared by dissolving Cu(ClO4)2·6H2O, Fe(ClO4)2, and Mg(ClO4)2, respectively, in THF. The resulting metal-ion solutions were gradually added to 5 × 10–5 M solutions of N-DBOV 10 or DBOV 11 in THF. Figure a and b reveal a significant decrease in the fluorescence intensity of N-DBOV 10 upon successive addition of Cu2+ (0–1.8 equiv) and Fe2+ (0–1.8 equiv) ions at room temperature. Indeed, N-DBOV 10 is highly sensitive to Cu2+ and Fe2+ ions, with a detection limit of 1 × 10–5 M, while DBOV 11 shows a much lower sensitivity (Figure c). According to the Stern–Volmer plot (Figure S38),[91,92] the quenching constant (KSV) of N-DBOV 10 was determined to be 3.4× 106 M–1 for Cu2+ detection and 3.3 × 106 M–1 for Fe2+ detection. In contrast to Cu2+ and Fe2+, the addition of Mg2+ ions did not significantly decrease the fluorescence intensity of N-DBOV 10 (Figure d), consistent with the quenching being caused by the interaction of metal ions with the N atoms of N-DBOV 10 through intermolecular charge transfer.[93] Therefore, N-DBOV 10 promises to be a selective sensor material for heavy metal ions with unique fluorescence properties that enable single-molecule imaging.

Figure 9

Changes in the fluorescence spectrum of 5 × 10–5 M N-DBOV 10 measured in THF solution at room temperature upon successive addition of (a) Cu2+, (b) Fe2+, and (d) Mg2+ ions; changes in the fluorescence spectrum of DBOV 11 upon gradual addition of (c) Cu2+ ions.

Conclusion

In summary, we have introduced N-DBOV 10 as a novel nanographene with nitrogen atoms incorporated into the zigzag edges; N-DBOV 10 exhibited a narrow energy gap and brilliant red luminescence with a high photoluminescence quantum yield of 76%. By virtue of nitrogen incorporation, N-DBOV 10 sensitively responded to protons as well as Cu2+ and Fe2+ ions, as indicated by clear changes in its absorption and/or fluorescence spectra. Moreover, N-DBOV 10 has excellent photophysical properties, such as high photostability and intrinsic blinking, which are beneficial for long-term 3D fluorescence imaging and super-resolution SMLM imaging, respectively. The combination of SMLM with the pH-dependent blinking properties of N-DBOV 10 can provide a way to determine pH differences at the nanoscale. Moreover, introduction of hydrophilic groups at the peripheral positions can potentially make N-DBOV 10 water-soluble[33,94] and thus provide very promising dyes not only in material analysis but also in biological systems. As such, purpose-oriented derivatization of DBOVs, for example, installment of binding functionality for biotargeting, can lead to new opportunities in modern imaging applications, which is currently pursued in our laboratories.