Yi
Yuan‡
a,
Mi
Chao‡
a,
Yunyi
Shang
a,
Yujia
Gao
a,
Guangle
Niu
*b,
Wanggang
Fang
c,
Liqing
He
*c and
Hui
Wang
*a
aKey Laboratory of Synthetic and Natural Functional Molecule Chemistry of the Ministry of Education, College of Chemistry & Materials Science, Northwest University, Xi’an 710127, China. E-mail: whui210@nwu.edu.cn
bSchool of Chemistry and Chemical Engineering, Beijing Institute of Technology, Beijing 100081, China. E-mail: niugl@bit.edu.cn
cNational Engineering & Technical Research Center on Pressure Vessels and Piping Safety, Hefei General Machinery Research Institute Co., Ltd, Hefei 230031, China. E-mail: heli_limao@163.com
First published on 8th November 2024
Developing multiple photoresponsive polymers is crucial for creating versatile intelligent materials; however, it poses a significant challenge due to the limited availability of photoactivated moieties. Herein, we present a novel series of dual photoresponsive spiro-[4,5]-cyclohexadiene-8-one polymers exhibiting photoactivated crosslinking and switch-on fluorescence behaviors. These polymers were synthesized through a robust palladium-catalyzed [2+2+1] cycloaddition polymerization reaction of 4-phenol diazonium tetrafluoroborate and diynes. Notably, the single photoreactive spiro-[4,5]-cyclohexadiene-8-one moiety endowed dual photoresponse features to these polymers. Upon UV irradiation, the cyclohexadienone moieties underwent a 2π+2π photocycloaddition reaction to form an insoluble crosslinked polymer network. Concurrently, the photoactivated fluorescence phenomenon of the crosslinked polymers was also observed. To our knowledge, these polymers represent the first examples of merging photocrosslinking and fluorescence turn-on properties into one single functional group. By harnessing the unique photocrosslinking and photoactivated fluorescence properties, we successfully imprinted 2D and 3D photopatterns for lithographic applications. These intriguing results provide an alternative design strategy of multiple photoresponsive polymers for fluorescent labelling and 2D/3D optical security.
Photocrosslinking polymers facilitate the information programming via mask and wash postprocessing, leading to insoluble 3D images upon illumination.13,14 Inspired by their common photoresponsive characteristics, we envisioned the possibility of designing a photochromic(switch)-integrated-photocrosslinking (PIP) polymer system to realize the 3D-encoding with the aid of mask assistant photocrosslinking technology as well as render the 2D-encoding using fluorochromic dyes. Coumarin15,16 and its derivatives17–19 equipped with carbonyl-activated carbon–carbon double bonds are one of the most widely utilized photocrosslinkable units (Fig. 1a), which are capable of undergoing reversible phototriggered 2π+2π cycloaddition with fast response and excellent thermal stability. The predominant approach for fabricating such systems is focused on integrating fluorochromic dyes into photoclickable polymer chains. However, the complexity of multistep preparation processes hampers their practicality in real samples.20,21 Given these challenges, the exploration and development of a novel polymer backbone containing a single specific functional group that combines both photocrosslinking and fluorochromic characteristics could offer a fresh perspective for composite polymers in the realm of 2D and 3D encoding applications.
Fig. 1 (a) Previous works on photocrosslinking of coumarin; (b) spiro[cyclopentane-naphthalen]-2′-one polymer by Tang; and (c) spiro-[4,5]-cyclohexadiene-8-one polymers in this work. |
In 2019, Tang's research group intelligently synthesized a series of spiro[cyclopentane-naphthalen]-2′-one polymers using a simple one-pot C–H activation/dearomatization strategy (Fig. 1b).22 The obtained spiro-polymers can be utilized to fabricate different well-resolved fluorescent photopatterns based on their photoinduced fluorescence switch properties. Moreover, the refractive index undergoes significant changes before and after irradiation, making them suitable for integrated silicon photon technology. What inspires us is that the fluorescence change originated from the photooxidation reaction, instead of the photocrosslinking reaction, between the carbonyl-activated carbon–carbon double bonds, which is typically different from the reported coumarin derivatives. In this respect, we designed and synthesized other spiro-cyclopentane naphthalenone polymer isomers to investigate whether the existence of the spiro-ring or the steric problem impacts the potential photocrosslinking properties and also explore the feasibility of novel PIP polymers through the spirocyclic scaffold.
In this study, we report the synthesis of a novel PIP polymer with the spiro-[4,5]-cyclohexadiene-8-one core through the A1 + B2 step polymerization employing easily accessible 4-phenol diazonium tetrafluoroborate and internal diynes. Notably, the resulting polymers exhibit rapid photocrosslinking capabilities to form dense networks and display photo-activated fluorescent turn-on properties upon exposure to 365 nm light. It is worth noting that these rigid polymers represent the first example of merging photocrosslinking and fluorescence turn-on properties into one single functional group. The unique dual-response behaviour, which is distinct from the 2-carbonyl isomer reported by the Tang group, is attributed to the 2π+2π cycloaddition reaction between spiro-[4,5]-cyclohexadiene-8-one moieties (Fig. 1c). This mechanism was corroborated through ultraviolet fluorescence spectra, 1H-NMR spectra, and infrared spectra. By harnessing the photocrosslinking capabilities and the alteration in the polymer's fluorescence properties upon irradiation, we succeeded in preparing 2D and 3D lithographic patterning using a simple method. Actually, for lithography, the photosensitive polymer development has experienced three different periods: the first one was the oil soluble polymer (also known as a negative resist), which contains many residual double bonds to facilitate crosslinking with other UV sensitive compounds (such as bisaryl azide).23 Upon radiation, the crosslinking took place and images with a resolution of microns became possible. However, due to the non-polar solvent usage for removal of the uncrosslinked regions, such materials suffer from swelling problems of the crosslinked regions and distortion of small features. The second one is the novolac-diazonaphthoquinone (DNQ) system (also known as a positive resist).24 The combined system was insoluble in an aqueous base; however, it became aqueous soluble upon irradiation due to the formation of a carboxylic acid as the photochemical rearrangement of DNQ. More recently, chemically amplified photoresists (CAR) composed of a poly(hydroxystyrene) polymer protected with a t-Boc group and combined with a photo-acid generator were invented by Willson, Fréchet and Ito.25 Upon exposure, the photo-acid generator releases a proton that can deprotect the polymer by release of t-Boc, which generates a high solubility contrast between the unexposed and protected polymers. All the mentioned photolithography techniques focus on the resolution of images and solubility of photo-responsive polymers, but little attention has been paid to the changes in fluorescence signals. Therefore, the proposed dual photoresponsive strategy in this study will provide a new idea for the photolithography techniques related to fluorescence changes.
In the first experiment, the optimized conditions for the synthesis of small molecule spiro-[4,5]decatetraene-8-one were adopted, that is, a 1:1 ratio of both monomers, the absence of base, and using 5 mmol% Pd(OAc)2 as a precatalyst in the presence of MeOH. However, only small molecules were obtained without any oligomer or polymer insolubles in the post-solution treatment (see Tables S1 and S2 in the ESI†). Despite temperature adjustments, the situation did not improve. Finally, we found that the poor solubility of diacetylene in methanol hindered the polymerization, prompting us to modify the reaction solvent to a mixed solvent, and successfully promoted the formation of the polymer in the mixed solution of dichloromethane (DCM) and methanol, which are good solvents for diacetylene and diazonium salt, respectively.
After identifying the optimal solvent system, we first examined the effects of catalyst and base loading on the polymerization of 1 (0.1 M) and 2a (0.1 M). As shown in entries 1–6 of Table 1, polymeric yellowish-brown solid P1/2a with high molecular weights (Mw = 14000) can be generated in a high yield of 91% when conducting the reaction in 5% mmol PdCl2 without the assistance of any base, which is consistent with the proposed mechanism of oxidative addition, double carbopalladation, aryl insertion and β-hydride elimination cascade process.26 To be noted, due to the asymmetric structure of the internal diyne, the chemical structure of P1/2a shown in Table 1 was supposed to be composed of regioisomers.
Entry | Catalyst | Solvent | [1]/[2a] (M) | T (h) | Temp. (°C) | Yield (%) | M w (g mol−1) | M n (g mol−1) | Đ | DPc |
---|---|---|---|---|---|---|---|---|---|---|
a Unless otherwise noted, [Pd] = 5 mmol %, DCM/MeOH with a 1/1 vol. ratio was used as the solvent. b Determined by GPC in THF on the basis of a polymethyl methacrylate calibration. Đ = polydispersity = Mw/Mn. c Degree of polymerization is determined by dividing the relative molecular weight (Mn) of the polymer by the molecular weight of its repeating unit. d NaOAc was added, [1]:[NaOAc] = 1:3. e [Pd] = 10%. f [Pd] = 20%. | ||||||||||
Screening of the catalysts and base | ||||||||||
1 | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 24 | 40 | 91 | 14000 | 5100 | 2.7 | 9 |
2 | Pd(OAc)2 | DCM:MeOH = 1:1 | 0.1/0.1 | 24 | 40 | 54 | 5300 | 1600 | 3.3 | 3 |
3 | Pd(CF3CO2)2 | DCM:MeOH = 1:1 | 0.1/0.1 | 24 | 40 | 44 | 3300 | 2800 | 1.2 | 5 |
4d | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 24 | 40 | 85 | 8400 | 4600 | 1.8 | 8 |
5d | Pd(OAc)2 | DCM:MeOH = 1:1 | 0.1/0.1 | 24 | 40 | 73 | 8900 | 3600 | 2.5 | 7 |
6d | Pd(CF3CO2) | DCM:MeOH = 1:1 | 0.1/0.1 | 24 | 40 | 69 | 7000 | 3700 | 1.9 | 7 |
Screening of temperature | ||||||||||
7 | PdCl2 | DCM:EtOH = 1:1 | 0.1/0.1 | 24 | 70 | 91 | 9500 | 2300 | 4.1 | 4 |
8 | PdCl2 | DCM:IPA = 1:1 | 0.1/0.1 | 24 | 70 | — | — | — | — | — |
9 | PdCl2 | DCM:TAA = 1:1 | 0.1/0.1 | 24 | 80 | — | — | — | — | — |
10 | PdCl2 | DCM:n-BuOH = 1:1 | 0.1/0.1 | 24 | 70 | — | — | — | — | — |
11 | PdCl2 | DCM:TFE = 1:1 | 0.1/0.1 | 24 | 40 | — | — | — | — | — |
12 | PdCl2 | DCM:HFIP = 1:1 | 0.1/0.1 | 24 | 40 | — | — | — | — | — |
Screening of monomer concentration | ||||||||||
13 | PdCl2 | DCM:MeOH = 1:1 | 0.15/0.15 | 24 | 40 | 76 | 6200 | 4100 | 1.5 | 8 |
14 | PdCl2 | DCM:MeOH = 1:1 | 0.05/0.05 | 24 | 40 | 88 | 11800 | 6200 | 1.9 | 12 |
15 | PdCl2 | DCM:MeOH = 1:1 | 0.15/0.1 | 24 | 40 | 90 | 12000 | 4500 | 2.7 | 8 |
16 | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.15 | 24 | 40 | 84 | 9990 | 4200 | 2.4 | 8 |
Screening of the reaction time and catalyst loading | ||||||||||
17 | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 48 | 40 | 89 | 15400 | 6700 | 2.3 | 13 |
18e | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 48 | 40 | 94 | 27400 | 16400 | 1.5 | 31 |
19f | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 48 | 40 | 69 | 10300 | 6300 | 1.6 | 12 |
20e | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 12 | 40 | 78 | 11600 | 9100 | 1.3 | 17 |
21e | PdCl2 | DCM:MeOH = 1:1 | 0.1/0.1 | 72 | 40 | 84 | 13400 | 9900 | 1.4 | 19 |
Next, the effects of temperature on the polymerization were investigated. The results shown in entries 7–12 suggested that variation of methanol to other high-boiling-point alcohols, such as IPA, TAA, and n-BuOH, or other polar protic solvents, including TFE or HFIP, completely halted the reaction. The only exception observed was with the DCM and EtOH mixture, which yielded a reduced polymerization efficiency with a degree of only 4. In this manner, DCM in combination with MeOH was still selected as the best mixture to adjust the temperature to 40 °C. As shown in entries 13–16, the relative proportions and absolute concentrations of the monomers 1 and 2a have a significant effect on the polymerization. Specifically, reducing the concentrations of both monomers 1 and 2a to 0.05 M leads to a moderate Mw of 11800 and a good polydispersity of 1.9. However, the nonstoichiometric proportion of the two monomers, such as 0.15/0.15 or 0.1/0.15, provided inferior results although the reaction can proceed smoothly. After the optimum catalyst, solvent, temperature, and monomer concentration were determined, the effects of catalyst equivalent and reaction time on polymerization were investigated. Satisfactorily, when the catalyst equivalent was increased to 10% and the reaction time was extended to 48 h, the target spiropolymer P1/2a was obtained with 93.7% yield, higher molecular weights (Mw = 27400, Mn = 16400) and a narrow polydispersity (Đ = 1.5).
Under the optimal conditions described above, we then studied the polymerization of diazonium salt with different internal diynes to enrich the polymer structures. As shown in Table 2, in addition to 2a–2c with different numbers (4–8) of flexible alkyl fragments, two rigid and conjugated internal alkynes were screened for the target polymerization, including dibenzothiophene-linked diyne 2d and triphenylamine-linked diyne 2e. Compared with the flexible alkynes with alkyl chains 2a–b, the reaction efficiency was decreased significantly due to the polyaromatic stiff linker of 2d–e as well as the highly rigid and twisted spiro-polymer, leading to oligomer P1/2d–e with a molar weight less than 10000 g mol−1. Interestingly, the efficiency of polymerization did not consistently improve with longer flexible alkyl chains. For example, for compound 2c with m equal to 8, the polymerization efficiency is significantly weakened, which may be related to the reduced probability of collisions between two acetylene molecules.
Entry | Polymer | Yield (%) | M w (g mol−1) | M n (g mol−1) | Đ | DPc |
---|---|---|---|---|---|---|
a Carried out in the presence of PdCl2 at 40 °C in DCM and MeOH under a nitrogen atmosphere for 48 h with [1] = [2] = 0.1 M and PdCl2 = 10 mol%. b Estimated by GPC in THF on the basis of polymethyl methacrylate calibration. Đ = polydispersity = Mw/Mn. c Degree of polymerization is determined by dividing the relative molecular weight (Mn) of the polymer by the molecular weight of its repeating unit. | ||||||
1 | P1/2a | 93.7 | 27400 | 16400 | 1.5 | 31 |
2 | P1/2b | 89.2 | 24100 | 13300 | 1.8 | 24 |
3 | P1/2c | 73.9 | 16000 | 7300 | 2.2 | 12 |
4 | P1/2d | 65.5 | 7900 | 3400 | 2.3 | 7 |
5 | P1/2e | 75.8 | 4500 | 2600 | 1.7 | 5 |
The structural characterization of model compound 4, spiropolymer P1/2a, and their corresponding monomers 1 and 2a is discussed here as a representative example for comparative analysis. The Fourier-transform infrared (FT-IR) and nuclear magnetic resonance (NMR) spectra were utilized as the major characterization method. As shown in Fig. 2, both the absorption bands related to stretching vibrations of the CC bond located at 2203 cm−1 of 2a in Fig. 2A and the NN bond located at 2230 cm−1 of 1 in Fig. 2B disappeared in Fig. 2C and D, indicating the reaction between the diazonium cation and the internal alkynes for the model reaction and polyannulation. New peaks emerged at 1650 cm−1, attributed to the stretching vibrations of the CO bond in Fig. 2C and D, demonstrating the occurrence of dearomatized spirocyclization and the presence of spiro-[4,5]-cyclohexadiene-8-one in 4 and P1/2a. Similarly, the other four spiropolymers P1/2b–e displayed similar characteristic variation to P1/2a (Fig. S1–S15 in the ESI†). The structural identity of the generated polymer P1/2a was confirmed by analysis of the 1H NMR spectra of product 4 in comparison with those of monomers 1 and 2a. As illustrated by the low-field region of the 1H-NMR spectra in Fig. 2E–H, the disappearance of broad Ha peaks (4.0–4.4 ppm) corresponding to the phenolic hydroxyl proton in monomer 1 (Fig. 2E) and appearance of downfield double peaks of Hd (6.43 ppm) both in model product 4 and polymer P1/2a (Fig. 2G and H) indicate the formation of the hexadienone moiety in the resulting spiropolymers. Moreover, the sharp peaks corresponding to alkane chains at δ 3.93 (Hb) and δ 1.90 (Hc) in polymer P1/2a remain as sharp as their monomer counterparts in 2a. This indicates the existence of flexible alkyl chains in polymer chains and confirms the occurrence of [2+2+1] cyclization between two equiv. of alkyne and azides to promote the formation of spirorings. The 13C-NMR analysis provides more detailed information on the polymer structure in Fig. 2I–L. The resonance peaks assigned to the acetylene carbon atoms (Ci) at δ 89.4 and 88.0 ppm and the hydroxyl carbon atom (Ch) at δ 175.62 ppm all disappeared in the spectrum of P1/2a. Instead, a new peak at δ 186.2 ppm emerged implying the formation of carbonyl groups in the polymer structure. The combination of 1H NMR and 13C NMR spectra of P1/2a largely resemble those of the model compound 4, confirming the successful synthesis of polymers with the structures shown in Table 1.
Considering the existence of the conjugated-π moiety and the brown colour of the obtained polymers, the photophysical properties of all the obtained spiropolymers were examined by UV-vis absorption and photoluminescence (PL) spectroscopy (Fig. 3C and D). As shown in Fig. 3C, P1/2a, P1/2b, P1/2c, P1/2d, P1/2e, and model compound 4 in dilute CHCl3 solution exhibited strong UV-vis absorption bands at 334, 332, 330, 343, 311 and 325 nm, respectively, assignable to the π–π* transitions resulting from the conjugation between the alkene moiety and the aromatic rings. Moreover, the energy bandgap evaluated from the tangential line of the long-wavelength absorption spectrum shows a decreasing trend as the π-conjugation length extended, especially for P1/2d and P1/2e. Upon UV irradiation at 345 nm in CHCl3, the maximum fluorescence emission appeared at 486–584 nm covering the blue, green and yellow regions. Compared to the λPL value of 405 nm exhibited by the model compound 4, all polymers displayed varying degrees of redshifted emission, influenced by their conjugation length. Specifically, as the conjugated structure increased in size and the attached aryl groups of the alkyne moiety enhanced its electron-donating capability, a more pronounced spectral bathochromic shift was observed, from P1/2c to P1/2d and further to P1/2e. This indicates the possible occurrence of intramolecular charge transfer, presumably arising from the homoconjugation between spiro-linked donor and acceptor moieties.32 However, when the compound P1/2a is transformed into a solid powder, its fluorescence is completely quenched, indicating that its PET mechanism may be activated in the solid state.33
Moreover, when a slightly higher concentration of P1/2a in THF (10 mg mL−1) was irradiated for 10 h, a black residue that was found to be insoluble in all organic solvents was obtained (Fig. 4B). All the phenomena suggest that the crosslinking of the polymer chains likely occurs via a 2π+2π cycloaddition reaction between the intermolecular carbon–carbon double bonds. Meanwhile, the degree of crosslinking (x) was calculated using the equation x = 1 − (At/A0), where A0 represents the initial absorbance and At represents the absorption value after a certain time of irradiation. Accordingly, the maximum crosslinking degree was estimated to be ∼67%, and this value remained almost unchanged from 60 to 240 minutes. Compared with the reported photoresponsive polymers, the reason for the low crosslinking degree may be related to the large steric hindrance between inter-chains caused by the rigid spiral scaffold. The attempt to enhance the crosslinking efficiency by changing the concentration proved futile. Despite our efforts to raise the concentration and increase the illuminance, the efficiency did not exhibit significant improvement (Fig. S17 in the ESI†). The plots of x against irradiation times for different polymers and solvents were also investigated, and the results are shown in Fig. S16 and S18 (ESI†). In the same solvent – THF, the cross-linking degree gradually declined as the alkyl chain length extended, ultimately reaching merely 45% for P1/2c. This reduction is likely strongly correlated with the decreased collision frequency of the activated carbon–carbon double bonds due to the increased flexibility of the alkyl chains. Furthermore, our findings indicate that changing the solvent had little impact on the maximum achievable crosslinking degree but instead primarily influenced the crosslinking speed, with chloroform solution exhibiting the highest crosslinking rate.
Besides UV-vis monitoring, 1H NMR spectroscopy and FT-IR spectroscopy were used to elucidate the mechanism for the intermolecular 2π+2π cycloaddition reaction. Initially, P1/2a were dissolved in CDCl3 at low concentrations (0.1 mg mL−1) and exposed to UV light (365 nm, 10 mW cm−2) in order to follow the chemical changes of the spirohexadienone moieties under irradiation. As shown in Fig. 4C, the 1H NMR spectra of P1/2a clearly display alkyl, aryl, and olefin proton signals with well-resolved peaks. After 60 minutes of UV irradiation, the resonance signal (δ 6.42 ppm) from the carbonyl-activated olefin protons noticeably weakened, and instead, new high-field signals (δ 3.21 ppm) corresponding to alkyl moieties emerged.34 This phenomenon suggested that the neighbouring alkenes, activated by the carbonyl in spiro-[4,5]-cyclohexadiene-8-one, might undergo intermolecular [2+2] cyclization, leading to the formation of rigid cyclobutane rings after irradiation and thus presenting apparent crosslinking. In addition, changes before and after irradiation were analyzed by FT-IR spectroscopy. As shown in Fig. 4D, the Vc=c at 1657 cm−1 assigned to the absorption of the olefinic bond in the spirohexadienone moiety of P1/2a disappeared after irradiation. The characteristic peak at 1589 cm−1, representing the carbonyl peak in P1/2a, shifted to a higher wave number of 1594 cm−1 due to the loss of conjugation. The combination of FT-IR, 1H NMR and UV-vis spectroscopy further confirmed the exact occurrence of 2π+2π cycloaddition for spiro-[4,5]-cyclohexadiene-8-one functionalized polymers; however, the crosslinking process for these spiro-polymers presented irreversibility nature when compared with traditional photoresponsive coumarin15 derivatives. After the UV-254 nm irradiation experiment [see the ESI†] and literature investigation, the competitive absorption of the spiro-polymer35 and higher energy for rigid crosslinking net restructuring36 are identified as the primary factors contributing to the irreversibility of the crosslinking process.
By successful demonstration of photocrosslinking, the viscoelastic characteristics of the crosslinked photocurable gels were thoroughly analyzed through oscillatory shear rheology conducted at 25 °C to determine their storage modulus (G′) and loss modulus (G′′) (Fig. 5A). The energy storage modulus (G′) values of the gels follow a descending order: P1/2a > P1/2b > P1/2c, indicating that the crosslinking density of P1/2a is the highest. At the same time, P1/2c exhibits a crossover point at a shear strain of 4.9%, demonstrating that the crosslinking network under such stress undergoes a breakdown.37 This observation further underscores the close correlation between the mechanical strength of the gel and the extent of crosslinking, revealing that a lower degree of crosslinking correlates with a more brittle gel. Next, frequency scanning was performed at a constant strain value of 0.1% in the linear viscoelastic region. As depicted in Fig. 5B, the energy storage modulus (G′) of the crosslinked polymer remained consistently higher than the loss modulus (G′′), indicating the presence of distinct gel-like structures as the two moduli remain independent of each other.38
On the basis of these results, the polymer concentration was further increased to study their gelation behavior. In order to select suitable gelation conditions, different concentrations were tested and 25 wt% was selected as the solubility limit for P1/2a–c. Subsequently, 25 wt% of the three polymers were dissolved in chloroform, and the solution was exposed to UV light at 365 nm for 24 hours to ensure complete cross-linking, and the residual solvent was removed using an oven. Next, the swelling test of these three organic gels was carried out in ethyl acetate to study their swelling behavior within 360 minutes (Fig. 5C and D). Calculated from eqn 1, the swelling ratios were 1.44, 0.82, and 0.4 g/g for P1/2c, P1/2b and P1/2a, respectively. The swelling results are in alignment with the principle that polymers with a high crosslinking density absorb a lower amount of solvent as a result of a smaller mesh size, reflecting the anti-swelling property of P1/2a gels.39
(1) |
As shown in Fig. 6A, photocrosslinking of the polymer film was conducted in air at room temperature (∼27 °C) for 60 minutes using 365 nm UV light with an intensity of 10 mW cm−2. The polymer film was prepared by dip-coating the polymer solution (30 wt% in CHCl3) onto a silicon wafer. The film was dried in a vacuum oven at room temperature overnight. The fluorescent image was generated using a black paper mask (Fig. 6B and C) or a Cu-negative mask (Fig. 6D) and taken using a digital camera or a fluorescent optical microscope (Olympus BX4) with a 330–385 nm broad range UV source.
Fig. 6 (A) Schematic diagram for photopatterning; the images for fluorescent patterning with a flower mask (B); “NWU” letter mask (C); and copper-negative microscopic mask (D) following the order of mask, UV on, UV off and after wash (notes: the size of all substrates is 2.5 cm × 2.5 cm. In Fig. 6B, the diameter of the flowers is 2.0 cm; each size of the “NMU” letters is 0.6 cm in Fig. 6C, and the diameter of the small circle is 100 microns in Fig. 6D). |
Indeed, upon exposure to UV light through black paper masks in the air for 60 minutes, the thin films of P1/2a underwent photocrosslinking, resulting in orange-red fluorescence in the exposed sections due to the blocked PET progress. In contrast, the masked regions, forming special images or letters, remained emission quenched (Fig. S19, ESI†). Consequently, 2D-fluorescent patterns were generated without the need for further development process. Notably, upon turning off the UV light, no mask patterns were observed on the surface of the films, suggesting potential applications of this photolithography process in the encryption field (see the UV-off images).
After the completion of 2D fluorescent patterning, we then immersed the exposed and patterned films into a dichloromethane solution. Since the masked regions were not photocrosslinking and could quickly dissolve in DCM, the masked pattern parts became concave, resulting in the immediate display of 3D-photolithographic patterns. Additionally, the polymers can also be used to fabricate microscopic maps with circular hole as small as 100 microns, typically, the sharp edges of the images can be clearly seen as shown in Fig. 6D. Therefore, the prepared spiro-polymers with exceptional solution processability present promising potential as 2D and 3D-encoding materials for utilization in optical display devices, optical writing and reading systems, as well as anti-counterfeiting applications.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4qm00688g |
‡ Y. Yuan and M. Chao contributed equally to this work. |
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