Tao
Yu
a,
Depei
Ou
a,
Leyu
Wang
a,
Shizhao
Zheng
a,
Zhiyong
Yang
a,
Yi
Zhang
*a,
Zhenguo
Chi
*a,
Siwei
Liu
a,
Jiarui
Xu
a and
Matthew P.
Aldred
b
aPCFM Lab, GD HPPC Lab, Guangdong Engineering Technology Research Center for High-Performance Organic and Polymer Photoelectric Functional Films, State Key Laboratory of Optoelectronic Material and Technologies, School of Chemistry and Chemical Engineering, Sun Yat-sen University, Guangzhou, 510275, P. R. China. E-mail: ceszy@mail.sysu.edu.cn; chizhg@mail.sysu.edu.cn
bDepartment of Chemistry, Durham University, DH1 3LE, UK
First published on 2nd June 2017
A carbazole containing triphenylethylene derivative (TrPEBCar) has been designed and synthesized, which combines aggregation-induced emission (AIE), piezochromism and photochromism together. In the crystalline state, an intensive emission band at 448 nm was detected. After pressing the crystalline solid, a [crystalline–amorphous] morphological transition takes place, in which the resulting amorphous state of TrPEBCar exhibits a different color and a red-shifted emission band at 470 nm. Photochromic behavior of TrPEBCar is achieved by utilizing a stilbene-type intramolecular photocyclization in the crystalline state. In addition, we report for the first time morphology-dependent photochromism, in which the photochromic properties of TrPEBCar are only observed in the crystalline state but not in the amorphous state. Therefore, the methods of pressing/fuming and heating/fuming act as gates to switch the photochromic properties by changing the aggregation states between the crystalline and amorphous states. By combining the piezochromic properties with the photochromic properties, the ON/OFF states of TrPEBCar can easily be observed by the different colors and emission properties. The triphenylethylene derivative with simple molecular structure provides a new approach for gated photochromic materials with both switch and indicator.
In recent years, there has been a growing interest regarding AIE-active materials, which can overcome the shortcomings of materials that exhibit significant fluorescence loss due to aggregation-caused quenching (ACQ).8 For AIE-active materials, emission intensities are significantly enhanced in the solid-state where the restriction of intramolecular rotation can efficiently occur. Several AIE-active molecular systems have been designed and developed, such as silole derivatives,9 tetraphenylethene derivatives,10 triphenylethylene derivatives11 and others.12 In addition, some interesting properties of AIE-active materials, such as self-assembling properties,13 piezochromic properties14 and very recently photochromic properties15 have also been discovered and investigated. For these piezochromic materials, the different aggregation states (crystalline or amorphous) can easily be altered and converted by pressing processes that is mainly attributed to the twisted packing structures of the AIE-active molecules. Subsequently, the colors and emission bands can be drastically altered.
Triphenylethylene derivatives have been investigated, separately, for their piezochromic and photochromic properties.14,15 Furthermore, the photochromic process of some previously reported triphenylethylene derivatives are associated with their aggregation states (crystalline or amorphous).15b In this regard, we envisaged that piezochromism and photochromism might be realized together in a triphenylethylene derivative with rational molecular design, and external stimuli could play as a switch to control the photochromic properties by changing the aggregation state. As previous literature reported, an electron withdrawing group in triphenylethylene derivatives could promote the photochromic process.1b,15 In addition, rigid and bulky groups might lead to the twisted packing mode in the solid-state and bring about the piezochromic phenomenon. Herein, we report two boronic acid pinacol ester containing AIE-active photochromic compounds TrPEB and TrPEBCar, as shown in Fig. 1. It was discovered that TrPEBCar exhibits multi-responsive properties (both photochromism and piezochromism) and AIE properties. Furthermore, the photochromic properties can be easily tuned by controlling the aggregation state (crystalline or amorphous). Thus, pressing/fuming and heating/fuming processes can influence the aggregation state and, consequently, act as gates to switch the photochromic properties. In addition, different colors and emission bands are observed in the crystalline and amorphous aggregation states. These features are able to promote real-time monitoring of the gated photochromic ON/OFF states.
= 208 nm. To further confirm the size of the nanoparticles, scanning electron microscopy (SEM) studies were performed with the same solution and is shown in the inset picture of Fig. 2(b). From the SEM results, the size of the nanoparticles were in accordance with the DLS data. To demonstrate the rotational properties of TrPEBCar in the dilute solution state and its effects on fluorescence properties, temperature-dependent emission studies (from 164.8 K to 273 K) were carried out for TrPEBCar in THF solution (Fig. 2(c)). At 164.8 K, a strong emission band can be detected, wherein the emission intensity decreases with increasing temperature. When the temperature increases to 273 K, negligible fluorescence is observed and the once prominent emission band has decreased so much to become indiscernible. These results are ascribed to the restriction of the intramolecular rotations and vibrations of TrPEBCar at low temperature and the blocking of the non-radiative decay processes. Similar results were also reported for other AIE-active molecules in the previous literature.9b In addition, the emission band mainly originates from the π–π* transition of TrPEBCar according to the previous reports.11a
To investigate the piezochromic properties of compounds TrPEB and TrPEBCar, emission spectra of non-pressed crystalline and pressed samples were recorded. For compound TrPEBCar piezochromism is observed. The emission maxima of TrPEBCar is red-shifted from 448 nm to 470 nm after pressing (Fig. 2(d)) and the color of the sample also changes from white to yellow, as shown in the inset pictures of Fig. 2(d). Consistent with the previous literature regarding AIE piezochromic materials, the piezochromic properties of TrPEBCar can be mainly attributed to its twisted molecular structure in the crystalline state.14a After pressing the sample, in which the crystalline state is converted to the amorphous state, the molecular configuration becomes more planar, which leads to a narrower π–π* energy gap.14 Differential scanning calorimetry (DSC) studies of TrPEBCar in the crystalline and amorphous states were carried out and the DSC scans are shown in Fig. S3 (ESI†). For the pressed sample a glass transition temperature (Tg) is detected at ca. 146 °C but not in the non-pressed crystalline sample, which reveals the aggregation state of TrPEBCar changes from a crystalline morphology to the amorphous state after pressing. The changes in morphology after pressing were further investigated by powder X-ray diffraction (pXRD) studies (vide infra). However, for compound TrPEB, no significant changes in the emission properties are observed after pressing. By comparing the structures of TrPEB and TrPEBCar, it can be concluded that the presence of the two bulky and rigid carbazole units bestows its piezochromic properties.
The ring-closing reaction of triphenylethylene derivatives are related to the aggregation state (crystalline or amorphous).15b For the bulky carbazole containing molecule TrPEBCar, the photochromism is quite different in the crystalline state compared to the amorphous state. We investigated the relationship between the photochromic properties and the morphology, in which photochromic studies of TrPEB and TrPEBCar were carried out with the samples in both crystalline and amorphous states and the UV-vis reflectance spectra recorded (Fig. S4–S7, ESI†). These results reveal that the photochromic process of TrPEB can be observed in both the crystalline state and amorphous state and is independent of morphology. However, on the contrary the photochromism of TrPEBCar just occurs in the crystalline state, not in the amorphous state and is, therefore, dependent on morphology. Although the amorphous state should be more disordered than the crystalline state, the molecules in the amorphous phase can be rigidly bound. There is evidence in the previous literature that planarization in triarylethylene-based materials takes place in the amorphous state compared to the crystalline state. This planarized conformation could enhance the packing and molecular rigidity,14 and consequently the restricted molecular conformations might prevent the necessary chemistry for ring closure taking place. This results in a loss of photochromism for TrPEBCar in the amorphous state. Combining this with the aforementioned piezochromic studies, pressing/fuming, heating/fuming are possible gates for the photochromic properties of TrPEBCar by switching the aggregation state between crystalline and amorphous. Therefore, these external stimuli could act as switches to turn off/turn on the photochromic properties of TrPEBCar. Fig. 4(a) demonstrates the process of turning off/turning on the photochromism using pressing/fuming as a switch. For the samples in the crystalline state, the color can be changed into red after irradiation, which is named photochromism ON-state. After pressing, no obvious color change is detected after irradiation indicating that the photochromism is in the OFF-state. In addition, the ON/OFF state can be easily distinguished by the color and emission properties of sample, as shown in Fig. 4(a). TrPEBCar in the OFF-state (pressed sample) is turned yellow and displays a red-shifted emission band, which is in accordance with the piezochromic properties. To further investigate the photochromic properties, temperature-dependent photochromic studies were performed for TrPEBCar both in the crystalline state and in the amorphous state (Fig. S9, ESI†). By gradually increasing the temperature, the photochromism of TrPECar in the crystalline state becomes weaker and finally undetectable. These results are mainly attributed to the unstable structure of the ring-closed form of TrPEBCar at elevated temperatures, according to the previous literatures.1b,2a For TrPEBCar in the amorphous state, no photochromism is observed at all the different temperatures. To further prove the photochromic properties are dependent on the aggregation state (crystalline or amorphous), UV-vis reflectance studies and XRD measurements were carried out for the TrPEBCar samples in different states: (1) sample in the crystalline state; (2) pressed sample; (3) sample in the crystalline state heated to 240 °C for 3 minutes; (4) pressed sample fumed with CH2Cl2 for 10 minutes; (5) sample in crystalline state heated to 240 °C for 3 minutes and fumed with CH2Cl2 for 10 minutes. The XRD spectra and UV-vis reflectance spectra of these samples are shown in Fig. 4(b and c), respectively. After pressing or heating, the peaks in the XRD pattern of TrPEBCar becomes more diffuse and less defined compared to the crystalline state. This indicates that most of the sample has been converted to the amorphous state from the crystalline state.17 Concurrently, negligible photochromic properties are observed in the amorphous state (OFF-state), which is shown in both the spectra and pictures in Fig. 4(a and c). For both the pressed sample and the heated sample, the XRD spectra becomes sharper and more defined after solvent fuming with dichloromethane, which subsequently turns on the photochromism (ON-state), as shown in Fig. 4(b and c). In addition, with regards to TrPEBCar the absorption and emission bands are quite different between the ON and OFF states of the gated photochromic material. Therefore, it is straightforward to conduct real-time monitoring of the ON/OFF states by distinguishing the color and emission properties.
Footnote |
| † Electronic supplementary information (ESI) available: Synthesis of TrPEB and TrPEBCar; physical measurements and instrumentations; DSC scans and UV-vis absorption/reflectance spectra. See DOI: 10.1039/c7qm00160f |
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