Aggregation-Induced Emission of Tetraphenylethene-Conjugated Phenanthrene Derivatives and Their Bio-Imaging Applications

In this study, a series of rationally designed emissive phenanthrene derivatives were synthesized and their aggregation-induced emission (AIE) properties in tetrahydrofuran (THF)/water mixtures were investigated. Two tetraphenylethene (TPE) segments were conjugated to both ends of the phenanthrene core at the para-positions and meta-positions, resulting in pTPEP and mTPEP derivatives, respectively. While the TPE-conjugated phenanthrene derivatives did not show any emission when dissolved in pure THF, they showed strong sky-blue emissions in water-THF mixtures, which is attributed to the restriction of intramolecular motions of TPE segments by aggregation. Furthermore, silica nanoparticles loaded with these AIE-active compounds were prepared and proved to be promising intracellular imaging agents.


Introduction
Several fluorescent nanoparticles with high emission efficiency have been developed in recent years for biological sensing and imaging applications [1]. Typically, emissive molecules have been synthesized using rigid planar aromatic cores because of their good thermal stability, long fluorescence lifetime, and high quantum yield [2,3]. However, conventional fluorescent molecules based on aromatic derivatives suffer from the aggregation caused quenching (ACQ) effect because of π-π stacking interactions in the planar fluorophores, which limits their applicability in organic light-emitting diode (OLED) materials or bio-imaging agents. Recently, Tang and co-workers have pioneered in studying a novel photophysical phenomenon i.e., aggregation-induced emission (AIE), which counteracts the typical effect of the ACQ process [4][5][6][7]. Mechanistic investigations have revealed that the AIE phenomenon is caused by the restriction of intramolecular rotations (IMR) of the luminogens in the aggregate states [8][9][10]. For instance, the four phenyl rings of tetraphenylethene (TPE) derivatives undergo an active IMR in the solution state and are thus non-emissive. In contrast, the IMR process of TPE derivatives is impeded in the aggregate state. Thus, the aggregation states prevent the non-radiative decay channel and elevate these compounds from faint fluorophores to strong blue light emitters [9,11,12]. Following this mechanism, many types of AIE luminogens have been synthesized. In particular, TPE possesses a simple structure but shows a magnificent AIE effect [10,13]. Therefore, TPE and its derivatives have been used to overcome the drawbacks of the ACQ effect and even been applied in biological sciences [8,14,15]. On the other hand, most of TPE derivatives are not soluble in the aqueous media, suggesting that their biological application is limited. However, the fluorescent probes can be made water-soluble and biocompatible by being placed inside nanocarriers such as silica nanoparticles.
Since the first successful synthesis of silica nanoparticles (SNPs) by a scientist working at Mobil [16,17], SNPs have become a promising choice for targeted drug delivery and medical imaging as they are non-toxic and demonstrate good biocompatibility and biodegradability [18,19]. Although SNPs are non-fluorescent, they can act as host materials for bio-imaging agents; fluorescent dyes can be introduced into the silica matrix via physical processes such as sol-gel process.
In this work, we synthesized AIE-active phenanthrene derivatives and investigated their photophysical properties and cell-imaging ability. We conjugated two TPE segments to both ends of the phenanthrene core at the para-positions and meta-positions to obtain the pTPEP and mTPEP derivatives, respectively. In particular, the phenanthrene has a rather rigid planar structure, thus increase the aggregation ability of their derivatives. The phenanthrene unit can be conjugated with two AIE segments at the para-position or meta-position, resulting in various AIE-active derivatives. Furthermore, phenanthrene-9,10-diol can be easily alkylated to increase the solubility of AIE-compound and their AIE actives were investigated in tetrahydrofuran (THF)/water mixtures with varying water fraction. The TPEP molecules were also encapsulated in silica nanoparticles. Notably, the entrapped TPEP compounds exhibited AIE behavior with a high emission intensity and the TPEP-loaded silica nanoparticles showed efficient cell-imaging ability. These novel AIE-active compounds and their loading onto silica nanoparticles may provide a useful strategy for the development of promising bio-imaging agents without ACQ.

Equipment
Absorption measurements were carried out on a Shimadzu UV-1650 PC spectrometer (Kyoto, Japan) in 1 cm quartz cuvette from 200 to 900 nm. Fluorescence spectra were obtained using a Hitachi F-7000 spectrometer (Tokyo, Japan). Solutions of a concentration of 10 µM were used for both absorption and fluorescence measurements at room temperature (∼25 • C). Absolute quantum yield measurements were carried out using an absolute photoluminescence (PL) quantum yield measurement system (C11347, Hamamatsu Photonics, Hamamatsu, Japan) equipped with a 150-W xenon lamp (Hamamatsu Photonics, Hamamatsu, Japan). All compounds were characterized by 1 H-NMR spectroscopy on a Bruker AM 250 spectrometer (Billerica, MA, USA). The purity of the products was checked by thin-layer chromatography (TLC, silica gel 60 mesh). The silica nanoparticles were detached by Eppendorf Centrifuge Model 5804. The size and morphology of silica nanoparticles were analyzed by using transmission electron microscopy (TEM) (JEOL, MA, USA). We used machine JEOL-JEM 2100F (Peabody, MA, USA) at an accelerating voltage of 200 kV. To prepare TEM samples, 0.001 wt.% solutions of silica nanoparticles were dropping onto holey carbon film copper. The solvent then was evaporated at room temperature.
Compounds 2 and 5 were synthesized using the same procedure. A representative example is described for compound 2. 2.75 g (5.98 mmol) of compound 1 and 3.67 g (21.08 mmol) of Na 2 S 2 O 4 were added in a mixture of THF/H 2 O (150/50 mL). The mixture was stirred at room temperature for 6 h then extracted with THF and H 2 O. The organic layer was filtered, dried over anhydrous magnesium sulfate then evaporated to get 2 (2.68 g, 97.1% yield). 1  Compounds 3 and 6 were synthesized using the same procedure. A representative example is described for compound 3. Compounds 2 (5.00 g, 10.82 mmol) was dissolved in DMSO (50 mL). After addition of 2.43 g (43.31 mmol) of pulverized potassium hydroxide, 6.14 g of methyl iodide was added dropwise under ice cooling over 20 mins. The mixture was stirred for 12 h at room temperature [23], then the resulting mixture was poured into 100 mL of water and extracted with diethyl ether. The organic phase was dried over anhydrous magnesium sulfate and filtered. The solvent was removed in a rotary evaporator. The crude product 3 was purified by column chromatography (dichloromethane: n-hexane by the ratio 2:1, v/v) to get yellow solid (3.03 g, 57.1% yield). 1

General Procedure for the Suzuki Coupling for the Preparation of pTPEP and mTPEP
TPE-boronic acid was synthesized according to the reported procedure [10]. In a 100 mL round bottom flask was placed on a mixture of compound 3 (500 mg, 1.02 mmol), Pd(PPh 3 ) 4 (50 mg, 0.043 mmol), TPE-B(OH) 2 (845 mg, 2.24 mmol) and K 2 CO 3 (1.38 g) with the mixture of toluene/ethanol/water by the ratio 40/5/5 mL under argon air. The reaction was refluxed for 12 h then being cooled to room temperature. The reactant mixture was washed three times by water and dichloromethane, dried over anhydrous magnesium sulfate and filtered then was concentrated by rotary evaporation. The pTPEP was purified by column chromatography, in which hexane/dichloromethane (3:1, v/v) was used as the eluent to obtain a white solid (505 mg, 55.1% yield). 1   Briefly, TPEP derivatives were loaded into silica nanoparticles (TPEP-SiO 2 ) according to the modified synthetic procedures [24]. In 100 mL round bottom flask, a mixture of 1 mL of TEOS, 32 mL of ethanol and 0.26 mL of TPEP derivatives solution in ethanol were added. The mixture was stirred for 1 h then the aqueous solution of NH 4 OH (25%, 1.5 mL) was added to the mixture and stirred for 36 h. Finally, the resulting mixtures were centrifuged at 10,000 rpm for 10 min and washed three times with distilled water.

Entrapment Efficiency
The entrapment efficiency was determined based on the calculation of amount of un-reacted TPEP derivatives in the supernatant. The concentration of free TPEP derivatives was calculated by UV spectrometer. Following the previously reported method [25], the entrapment efficiency (E %) was confirmed by Equation (1)

Photostability of Nanoparticles
To study the photostability of free TPEP derivatives, a 3.5 mL of EtOH solution contains 1 mg of TPEP derivatives which was putted in a quartz cuvette in the dark at the room temperature. The TPEP-loaded silica nanoparticles were also prepared with the similar concentration condition in EtOH solution. Photobleaching experiments were carried out by irradiating the samples with Xe lamp (150 W, Abet Technologies, Milford, CT, USA). At every 10 mins of irradiation, the absorption spectra of each sample were measured by UV-Vis spectrophotometer.

Cell Culture and Bio-Imaging Experiment
To assess the cellular uptake and imaging abilities of mTPEP-SiO 2 and pTPEP-SiO 2 nanoparticles, HeLa (human cervix adenocarcinoma) was obtained from the American Type Culture and Collection and cultured in Dulbecco's modified Eagle's medium (DMEM, Welgene, Gyeongsangbuk-do, South Korea) with 10% fetal bovine serum (FBS, Welgene, Gyeongsangbuk-do, South Korea) and 1% penicillin-streptomycin under a humidified atmosphere (containing 5% CO 2 and 95% air) at 37 • C. Pre-cultured HeLa cell was plated in a 24-well cell culture plate at 1 × 10 5 cells/mL and incubated at 37 • C in 5% CO 2 for 24 h [26]. After incubation, the media of each well in the plate were changed with fresh media and further incubated with 40 µg/mL of mTPEP-SiO 2 and pTPEP-SiO 2 nanoparticles for 2 h in the dark condition. Finally, the plate was washed three times with Dulbecco's phosphate buffered saline (DPBS, Welgene, Gyeongsangbuk-do, South Korea) to remove remained silica nanoparticles before cellular imaging [27]. The morphology of HeLa cells was observed under an automated live cell imager (Lionheart FX, BioTek Instruments, Inc., Winooski, VT, USA) with 20× objective lens and fluorescence optics (excitation at 377 nm and emission at 447 nm).

Synthesis and Optical Properties
Scheme 1 outlines the synthesis of TPEP derivatives consisting of a phenanthrene moiety and two TPE units. The two TPE segments were conjugated to both ends of the phenanthrene core in the para-positions and meta-positions to obtain pTPEP and mTPEP, respectively. The synthesis of the aromatic core started with the halogenation of phenanthrenequinone to yield intermediates 2,7-diiodophenanthrenequinone (1) and 3,6-dibromophenanthrenequinone (4), which were then reduced to 2,7-diiodophenanthrene-9,10-diol (2) and 3,6-dibromophenanthrene-9,10-diol (5), respectively, using sodium hydrosulfite. The etherification of 2 and 5 with iodomethane in the presence of potassium hydroxide was performed and subsequent Sonogashira reactions with TPE-boronic acid produced the pTPEP and mTPEP derivatives, respectively. the aromatic core started with the halogenation of phenanthrenequinone to yield intermediates 2,7-diiodophenanthrenequinone (1) and 3,6-dibromophenanthrenequinone (4), which were then reduced to 2,7-diiodophenanthrene-9,10-diol (2) and 3,6-dibromophenanthrene-9,10-diol (5), respectively, using sodium hydrosulfite. The etherification of 2 and 5 with iodomethane in the presence of potassium hydroxide was performed and subsequent Sonogashira reactions with TPE-boronic acid produced the pTPEP and mTPEP derivatives, respectively. The photophysical properties of the TPEP derivatives were investigated in various solvents. The mTPEP compound shows absorption peaks (λab) in the range of 329-336 nm, which are slightly red-shifted with an increase in the solvent polarity but not significant (Table 1). On the other hand, the pTPEP compound exhibits two main absorption peaks. The higher-energetic peaks observed in the 308-312 nm region could be assigned to the local transition of the phenanthrene core while the lower-energetic peaks in the region 345-355 nm were attributed to the fully delocalized π-π* transition between the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) of pTPEP [2]. The overall red-shifted absorption of pTPEP as compared to that of mTPEP is likely responsible for the 1-dimensionally extended π-conjugation of the para-linked TPE segments mediated through phenanthrene core relative to their counterpart with the meta-linked TPEs [28]. The photophysical properties of the TPEP derivatives were investigated in various solvents. The mTPEP compound shows absorption peaks (λ ab ) in the range of 329-336 nm, which are slightly red-shifted with an increase in the solvent polarity but not significant (Table 1). On the other hand, the pTPEP compound exhibits two main absorption peaks. The higher-energetic peaks observed in the 308-312 nm region could be assigned to the local transition of the phenanthrene core while the lower-energetic peaks in the region 345-355 nm were attributed to the fully delocalized π-π* transition between the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) of pTPEP [2]. The overall red-shifted absorption of pTPEP as compared to that of mTPEP is likely responsible for the 1-dimensionally extended π-conjugation of the para-linked TPE segments mediated through phenanthrene core relative to their counterpart with the meta-linked TPEs [28]. The luminescence behaviors of the TPEP derivatives varied dramatically on varying the solvents in contrast to their UV-Vis spectra. Upon excitation by UV light at 365 nm, the TPEP derivatives in non-polar hexane displayed yellow-green emissions (Figure 1), which were deep blue in relatively polar solvents such as dichloromethane and nearly invisible in polar media such as THF and ethanol. In their emission spectra, the TPEP derivatives showed multi-peaks at 380-410 nm, which reduced in intensity as the solvent polarity increased ( Figure 2). The TPE units are well-known for poor fluorescence in their dissolved states because of the loss of excitation energy by IMR of the four phenyl rings [2]. Similarly, in this study, the multiple phenyl rings in the isolated molecules of mTPEP and pTPEP luminogens underwent active IMR, which effectively annihilated their excited states and rendered them non-emissive [7,8,[29][30][31]. Notably, a strong peak appeared at~480 nm in the non-polar hexane solution corresponding to the emission from aggregated TPE units. The low solubility of the TPEP derivatives in hexane seems to cause the aggregation of TPE units. The restrain on IMR of TPE units due to their aggregation enhanced the emission intensity at~480 nm, suggesting that the TPEP compounds exhibited AIE behavior in hexane solution. The luminescence behaviors of the TPEP derivatives varied dramatically on varying the solvents in contrast to their UV-Vis spectra. Upon excitation by UV light at 365 nm, the TPEP derivatives in non-polar hexane displayed yellow-green emissions (Figure 1), which were deep blue in relatively polar solvents such as dichloromethane and nearly invisible in polar media such as THF and ethanol. In their emission spectra, the TPEP derivatives showed multi-peaks at 380-410 nm, which reduced in intensity as the solvent polarity increased (Figure 2). The TPE units are well-known for poor fluorescence in their dissolved states because of the loss of excitation energy by IMR of the four phenyl rings [2]. Similarly, in this study, the multiple phenyl rings in the isolated molecules of mTPEP and pTPEP luminogens underwent active IMR, which effectively annihilated their excited states and rendered them non-emissive [7,8,[29][30][31]. Notably, a strong peak appeared at ~480 nm in the non-polar hexane solution corresponding to the emission from aggregated TPE units. The low solubility of the TPEP derivatives in hexane seems to cause the aggregation of TPE units. The restrain on IMR of TPE units due to their aggregation enhanced the emission intensity at ~480 nm, suggesting that the TPEP compounds exhibited AIE behavior in hexane solution.

AIE Properties
To further confirm the AIE properties of the TPEP derivatives, we investigated their optical properties in THF/water mixtures having different water fractions. Since TPEP derivatives are not soluble in water, they aggregated in the THF/water solutions with high water fractions. As shown in the photographs of the THF/water solutions of the TPEP derivatives taken under UV illumination (365 nm) (Figure 3), the colors became deep blue when the water fraction increased to 60% and turned strong sky blue when the volume of water was 90%. The emission profiles of the TPEP compounds were consistent with their corresponding photographs. Almost no emission signal could be detected from the TPEP compounds in pure THF. When the water fraction was 60%, the emission peaks at ~380-410 nm became stronger (Figure 4). This was attributed to the enhanced hydrophobicity of the media because of the aggregation of the TPEP compounds in the poor solvent (water). Strong emissions at ~480 nm were observed when the water fraction reached 70%, which intensified ~51 and 27-fold, respectively for mTPEP and pTPEP when the water fraction was 90% as compared to the emissions from pure THF solutions. These results confirmed that the TPE segments started to aggregate in solutions comprising over 70% of water, resulting in the restriction of the IMR of TPE units that caused AIE.

AIE Properties
To further confirm the AIE properties of the TPEP derivatives, we investigated their optical properties in THF/water mixtures having different water fractions. Since TPEP derivatives are not soluble in water, they aggregated in the THF/water solutions with high water fractions. As shown in the photographs of the THF/water solutions of the TPEP derivatives taken under UV illumination (365 nm) (Figure 3), the colors became deep blue when the water fraction increased to 60% and turned strong sky blue when the volume of water was 90%.

AIE Properties
To further confirm the AIE properties of the TPEP derivatives, we investigated their optical properties in THF/water mixtures having different water fractions. Since TPEP derivatives are not soluble in water, they aggregated in the THF/water solutions with high water fractions. As shown in the photographs of the THF/water solutions of the TPEP derivatives taken under UV illumination (365 nm) (Figure 3), the colors became deep blue when the water fraction increased to 60% and turned strong sky blue when the volume of water was 90%. The emission profiles of the TPEP compounds were consistent with their corresponding photographs. Almost no emission signal could be detected from the TPEP compounds in pure THF. When the water fraction was 60%, the emission peaks at ~380-410 nm became stronger (Figure 4). This was attributed to the enhanced hydrophobicity of the media because of the aggregation of the TPEP compounds in the poor solvent (water). Strong emissions at ~480 nm were observed when the water fraction reached 70%, which intensified ~51 and 27-fold, respectively for mTPEP and pTPEP when the water fraction was 90% as compared to the emissions from pure THF solutions. These results confirmed that the TPE segments started to aggregate in solutions comprising over 70% of water, resulting in the restriction of the IMR of TPE units that caused AIE. The emission profiles of the TPEP compounds were consistent with their corresponding photographs. Almost no emission signal could be detected from the TPEP compounds in pure THF. When the water fraction was 60%, the emission peaks at~380-410 nm became stronger (Figure 4). This was attributed to the enhanced hydrophobicity of the media because of the aggregation of the TPEP compounds in the poor solvent (water). Strong emissions at~480 nm were observed when the water fraction reached 70%, which intensified~51 and 27-fold, respectively for mTPEP and pTPEP when the water fraction was 90% as compared to the emissions from pure THF solutions. These results confirmed that the TPE segments started to aggregate in solutions comprising over 70% of water, resulting in the restriction of the IMR of TPE units that caused AIE.

Size Determination
We also prepared silica nanoparticles containing TPEP compounds via a one-pot synthesis method to investigate their AIE behaviors within silica matrix in water. The TPEP-loaded silica nanoparticles, TPEP-SiO2, were prepared by hydrolysis and condensation of TEOS in the presence of alcoholic TPEP solution. The TEM images showed that the synthesized SiO2 nanoparticles were spherical with a narrow size distribution from 110 to 130 nm ( Figure 5). Additionally, it was found that the size and morphology of both mTPEP-loaded and pTPEP-loaded nanoparticles were very similar. The entrapment efficiencies of the TPEP compounds in the SiO2 nanoparticles were calculated using Equation (1). The entrapment yields of TPEP derivatives were calculated to be 99.1% and 99.8% for mTPEP-SiO2 and pTPEP-SiO2, respectively. Also, the loading efficiencies of the TPE derivatives into the nanoparticles were ~0.77% w/w and 0.87% w/w of the total weight of the nanoparticles for mTPEP-SiO2 and pTPEP-SiO2, respectively. Importantly, mTPEP-SiO2 and mTPEP-SiO2 in aqueous solutions exhibited strong emissions at 477 nm and 482 nm, respectively, as shown in Figure 6, which was the same as the results observed for TPEP derivatives in THF/water mixture. Fluorescence quantum yields of mTPEP-SiO2 and pTPEP-SiO2 increased up to 0.191 and 0.176, respectively. This result suggests that the TPEP derivatives aggregated inside the silica matrix and formed the AIE-active silica nanoparticles in the aqueous solution.

Size Determination
We also prepared silica nanoparticles containing TPEP compounds via a one-pot synthesis method to investigate their AIE behaviors within silica matrix in water. The TPEP-loaded silica nanoparticles, TPEP-SiO 2 , were prepared by hydrolysis and condensation of TEOS in the presence of alcoholic TPEP solution. The TEM images showed that the synthesized SiO 2 nanoparticles were spherical with a narrow size distribution from 110 to 130 nm ( Figure 5). Additionally, it was found that the size and morphology of both mTPEP-loaded and pTPEP-loaded nanoparticles were very similar. The entrapment efficiencies of the TPEP compounds in the SiO 2 nanoparticles were calculated using Equation (1). The entrapment yields of TPEP derivatives were calculated to be 99.1% and 99.8% for mTPEP-SiO 2 and pTPEP-SiO 2 , respectively. Also, the loading efficiencies of the TPE derivatives into the nanoparticles were~0.77% w/w and 0.87% w/w of the total weight of the nanoparticles for mTPEP-SiO 2 and pTPEP-SiO 2 , respectively. Importantly, mTPEP-SiO 2 and mTPEP-SiO 2 in aqueous solutions exhibited strong emissions at 477 nm and 482 nm, respectively, as shown in Figure 6, which was the same as the results observed for TPEP derivatives in THF/water mixture. Fluorescence quantum yields of mTPEP-SiO 2 and pTPEP-SiO 2 increased up to 0.191 and 0.176, respectively. This result suggests that the TPEP derivatives aggregated inside the silica matrix and formed the AIE-active silica nanoparticles in the aqueous solution.

Size Determination
We also prepared silica nanoparticles containing TPEP compounds via a one-pot synthesis method to investigate their AIE behaviors within silica matrix in water. The TPEP-loaded silica nanoparticles, TPEP-SiO2, were prepared by hydrolysis and condensation of TEOS in the presence of alcoholic TPEP solution. The TEM images showed that the synthesized SiO2 nanoparticles were spherical with a narrow size distribution from 110 to 130 nm ( Figure 5). Additionally, it was found that the size and morphology of both mTPEP-loaded and pTPEP-loaded nanoparticles were very similar. The entrapment efficiencies of the TPEP compounds in the SiO2 nanoparticles were calculated using Equation (1). The entrapment yields of TPEP derivatives were calculated to be 99.1% and 99.8% for mTPEP-SiO2 and pTPEP-SiO2, respectively. Also, the loading efficiencies of the TPE derivatives into the nanoparticles were ~0.77% w/w and 0.87% w/w of the total weight of the nanoparticles for mTPEP-SiO2 and pTPEP-SiO2, respectively. Importantly, mTPEP-SiO2 and mTPEP-SiO2 in aqueous solutions exhibited strong emissions at 477 nm and 482 nm, respectively, as shown in Figure 6, which was the same as the results observed for TPEP derivatives in THF/water mixture. Fluorescence quantum yields of mTPEP-SiO2 and pTPEP-SiO2 increased up to 0.191 and 0.176, respectively. This result suggests that the TPEP derivatives aggregated inside the silica matrix and formed the AIE-active silica nanoparticles in the aqueous solution.

Photobleaching
The photostability of silica nanoparticles is also important as they are to be used as bio-imaging agents in complex physiological environments [32]. In this respect, to verify the photostability of the prepared emissive silica nanoparticles, the photo-degradation experiments of TPEP-SiO2 nanoparticles and pure compounds were carried out under Xe lamp irradiation (150 W) three times. Figure 7 shows the photobleaching behavior of the TPEP-SiO2 nanoparticles and free TPEP derivatives. After 80 min of irradiation of the Xe lamp, the fluorescence intensity of pTPEP and mTPEP compounds decreased to 58% and 64%, respectively, compared to the initial intensity. On the other hand, the TPEP-SiO2 nanoparticles did not show any obvious changes in fluorescence intensity even after continuous Xe lamp irradiation for 80 min. From the observed results, it was evident that the TPEP-SiO2 nanoparticles had high photostability. The silica matrix can protect the encapsulated TPEP molecules by making them inaccessible to the solvent and reduce their oxidation by lowering the diffusion rate of oxygen, which results in the enhanced photostability. Furthermore, the aggregation of TPEP molecules could prevent further photobleaching and photo-oxidation by preventing oxygen diffusion into the nanoaggregates within the silica matrix [27]. These results indicate that the TPEP derivatives encapsulated in the silica matrix have enhanced the potential for bio-imaging applications because a high photostability of fluorescent probes benefits their long-term cell imaging.

Photobleaching
The photostability of silica nanoparticles is also important as they are to be used as bio-imaging agents in complex physiological environments [32]. In this respect, to verify the photostability of the prepared emissive silica nanoparticles, the photo-degradation experiments of TPEP-SiO 2 nanoparticles and pure compounds were carried out under Xe lamp irradiation (150 W) three times. Figure 7 shows the photobleaching behavior of the TPEP-SiO 2 nanoparticles and free TPEP derivatives. After 80 min of irradiation of the Xe lamp, the fluorescence intensity of pTPEP and mTPEP compounds decreased to 58% and 64%, respectively, compared to the initial intensity. On the other hand, the TPEP-SiO 2 nanoparticles did not show any obvious changes in fluorescence intensity even after continuous Xe lamp irradiation for 80 min. From the observed results, it was evident that the TPEP-SiO 2 nanoparticles had high photostability. The silica matrix can protect the encapsulated TPEP molecules by making them inaccessible to the solvent and reduce their oxidation by lowering the diffusion rate of oxygen, which results in the enhanced photostability. Furthermore, the aggregation of TPEP molecules could prevent further photobleaching and photo-oxidation by preventing oxygen diffusion into the nanoaggregates within the silica matrix [27]. These results indicate that the TPEP derivatives encapsulated in the silica matrix have enhanced the potential for bio-imaging applications because a high photostability of fluorescent probes benefits their long-term cell imaging.

Photobleaching
The photostability of silica nanoparticles is also important as they are to be used as bio-imaging agents in complex physiological environments [32]. In this respect, to verify the photostability of the prepared emissive silica nanoparticles, the photo-degradation experiments of TPEP-SiO2 nanoparticles and pure compounds were carried out under Xe lamp irradiation (150 W) three times. Figure 7 shows the photobleaching behavior of the TPEP-SiO2 nanoparticles and free TPEP derivatives. After 80 min of irradiation of the Xe lamp, the fluorescence intensity of pTPEP and mTPEP compounds decreased to 58% and 64%, respectively, compared to the initial intensity. On the other hand, the TPEP-SiO2 nanoparticles did not show any obvious changes in fluorescence intensity even after continuous Xe lamp irradiation for 80 min. From the observed results, it was evident that the TPEP-SiO2 nanoparticles had high photostability. The silica matrix can protect the encapsulated TPEP molecules by making them inaccessible to the solvent and reduce their oxidation by lowering the diffusion rate of oxygen, which results in the enhanced photostability. Furthermore, the aggregation of TPEP molecules could prevent further photobleaching and photo-oxidation by preventing oxygen diffusion into the nanoaggregates within the silica matrix [27]. These results indicate that the TPEP derivatives encapsulated in the silica matrix have enhanced the potential for bio-imaging applications because a high photostability of fluorescent probes benefits their long-term cell imaging.

TPEP-SiO 2 for Cell Imaging
To investigate the effectiveness of the fluorescent nanoparticles for cellular imaging, HeLa cells were treated with the TPEP-encapsulated nanoparticles. Sky blue-colored emission was observed when the loaded nanoparticles were excited at 377 nm as shown in Figure 8B,E. The images in Figure 8B,E show the cellular uptake and intracellular distribution of mTPEP-SiO 2 and pTPEP-SiO 2 and exhibit the successful cellular imaging of the HeLa cells without any morphological change and cytotoxicity for 2 h. This result is consistent with the reported nano-silica characteristics. Based on this result, it was evident that the mTPEP and pTPEP encapsulated inside silica nanoparticles would be useful as materials for cellular imaging.

TPEP-SiO2 for Cell Imaging
To investigate the effectiveness of the fluorescent nanoparticles for cellular imaging, HeLa cells were treated with the TPEP-encapsulated nanoparticles. Sky blue-colored emission was observed when the loaded nanoparticles were excited at 377 nm as shown in Figure 8B,E. The images in Figure 8B,E show the cellular uptake and intracellular distribution of mTPEP-SiO2 and pTPEP-SiO2 and exhibit the successful cellular imaging of the HeLa cells without any morphological change and cytotoxicity for 2 h. This result is consistent with the reported nano-silica characteristics. Based on this result, it was evident that the mTPEP and pTPEP encapsulated inside silica nanoparticles would be useful as materials for cellular imaging.

Conclusions
In conclusion, TPE-modified phenanthrene derivatives were synthesized and their solvent-dependent AIE properties were investigated. Two TPE units were conjugated to both ends of the phenanthrene core at the meta-positions and para-positions to obtain mTPEP and pTPEP derivatives, respectively. Investigation of the photophysical properties revealed that the TPEP derivatives exhibited AIE properties in the THF/water mixtures; the derivatives emitted strong sky-blue light until the fraction of water reached up to 90%. This was attributed to the suppressed rotation of the four phenyl rings of the TPE units, which prevented the non-radiative decay process and increased the emission intensity. Furthermore, the two TPEP compounds were encapsulated into silica nanoparticles; they adopted a spherical shape and were mono-disperse with diameters ranging ~110 nm. The TPEP-loaded silica nanoparticles emitted strong sky-blue emission in aqueous solutions and fluorescently visualized HeLa cells because AIE-activity of the TPEP compounds was also achieved within the silica matrix. Notably, the silica matrix acts as a protective shield, enhancing the photostability of the entrapped AIE compounds. Thus, these novel AIE-active compounds and their loading onto silica nanoparticles may provide a useful strategy for the development of promising bio-imaging agents without ACQ behavior.

Conclusions
In conclusion, TPE-modified phenanthrene derivatives were synthesized and their solvent-dependent AIE properties were investigated. Two TPE units were conjugated to both ends of the phenanthrene core at the meta-positions and para-positions to obtain mTPEP and pTPEP derivatives, respectively. Investigation of the photophysical properties revealed that the TPEP derivatives exhibited AIE properties in the THF/water mixtures; the derivatives emitted strong sky-blue light until the fraction of water reached up to 90%. This was attributed to the suppressed rotation of the four phenyl rings of the TPE units, which prevented the non-radiative decay process and increased the emission intensity. Furthermore, the two TPEP compounds were encapsulated into silica nanoparticles; they adopted a spherical shape and were mono-disperse with diameters ranging~110 nm. The TPEP-loaded silica nanoparticles emitted strong sky-blue emission in aqueous solutions and fluorescently visualized HeLa cells because AIE-activity of the TPEP compounds was also achieved within the silica matrix. Notably, the silica matrix acts as a protective shield, enhancing the photostability of the entrapped AIE compounds. Thus, these novel AIE-active compounds and their loading onto silica nanoparticles may provide a useful strategy for the development of promising bio-imaging agents without ACQ behavior.