Zhibin
Li
,
Ying
Zhang
,
Lirong
Zhu
,
Tao
Shen
and
Huiqi
Zhang
*
Key Laboratory of Functional Polymer Materials (Nankai University), Ministry of Education, Department of Chemistry, Nankai University, Tianjin, 300071, P. R. China. E-mail: zhanghuiqi@nankai.edu.cn; Fax: +86-2223507193; Tel: +86-2223507193
First published on 16th August 2010
A new and highly efficient approach to obtaining high molecular weight (up to 303000) azobenzene (azo)-containing side-chain liquid crystalline polymers by copper(I)-catalyzed polymer analogous click chemistry is described. A series of azo compounds with an azido end group and different flexible spacers were successfully attached onto a polymer bearing pendant acetylene groups (i.e., poly(propargyl methacrylate)) in rather high functionalization efficiency (≥97%). The chemical structures, phase transition behaviors, and photoresponsivity of the obtained polymers were characterized, and they were also compared with those of the corresponding low molecular weight azo polymers (prepared via conventional free radical polymerization) to study the effects of the largely different molecular weights on the properties of the polymers. Both the high and low molecular weight azo polymers with a flexible spacer = (CH2)10 showed smectic C liquid crystallinity and an increase in the molecular weight led to a broader range of the liquid crystalline phase, which is positive for potential applications. Furthermore, the highly reversible photoisomerization of the polymer solutions was proven to be hardly affected by the increase of the molecular weights.
The azo-containing side-chain LCPs have been mostly prepared via free radical polymerization because of its tolerance to a wide range of functional groups and mild reaction conditions. Unfortunately, the molecular weights of the resulting polymers are generally rather low (normally ranging from a few to tens of thousands) due to the large steric hindrance of the azo monomers, which results in their poor mechanical properties and thus severely limits their application for fabricating robust optical and optoelectronic devices. Therefore, an effective approach to generating high molecular weight azo-containing side-chain LCPs is highly desirable. In this respect, the polymer analogous reaction approach appears to be a useful solution to this problem, which involves the first preparation of a precursor polymer with reactive groups and its subsequent coupling with an azo compound bearing a corresponding reactive group. The flexibility in the preparation of high molecular weight precursor polymers via free radical polymerization (or other polymerization techniques), together with the availability of many different types of efficient coupling reactions,20 makes the polymer analogous reaction approach a highly versatile route for obtaining high molecular weight polymers with desired functional groups. So far, many relatively high molecular weight azo polymers have been successfully prepared by attaching azo mesogens to the preformed polymer backbones.21–26 The polymer analogous esterification reaction between a polymer bearing carboxyl chloride (or hydroxyl) groups and an azo compound with a hydroxyl (or carboxyl chloride) group appears to be one of the most efficient methods in terms of the high functionalization efficiencies.23,24 However, the use of carboxyl chloride in the above system requires fully anhydrous reaction conditions in order to achieve a functionalization degree close to 100%, which prevents it from being applied in aqueous media. Therefore, new and versatile synthetic strategies still need to be explored.
Recent years have witnessed an ever-increasing interest in the “click” chemistry because of its remarkable features such as its tolerance to a large number of functional groups, mild reaction conditions (the presence of water is allowed), and nearly quantitative yields.27–29 In particular, the copper(I)-catalyzed Huisgen 1,3-dipolar cycloaddition reaction between azides and alkynes has proven to be one of the most powerful click reactions and it has been successfully applied in the field of polymer science, affording a variety of functional polymer materials such as block polymers, dendrimers, and many other complex macromolecular structures.30,31 Very recently, a number of azo-containing functional polymers have been prepared via copper(I)-catalyzed click chemistry.32–41 Haddleton and coworkers prepared a series of azo group end-capped polymers by the polymer analogous click reaction between azido terminally functionalized poly(methyl methacrylate)s and an azo compound bearing an alkyne group.32 Liu and coworkers reported the successful synthesis of triazole-linked azo dendrons via repetitive click reactions between a diazido functionalized azobenzene and a monoalkyne functionalized azobenzene with two chloroethyl groups.33 Li and coworkers prepared a series of azo-containing nonlinear optical polymers via copper(I)-catalyzed polymer analogous click chemistry.34–36 Zhu and coworkers described the preparation of some main-chain azo polymers via step-growth polymerization based on click chemistry.37,38 Kannan and coworkers reported the synthesis of a series of side-chain LCPs with triazole-substituted azo groups by conventional free radical polymerization of the corresponding azo monomers (which were prepared via click chemistry).39 The groups of Oriol and Sánchez reported the preparation of a series of azo-containing linear-dendritic diblock copolymers by click chemistry.40,41 To the best of our knowledge, however, there have been no reports on the synthesis of azo-containing side-chain LCPs via copper(I)-catalyzed polymer analogous click chemistry up to now.
In this paper, we present the efficient synthesis of photoresponsive azo-containing side-chain LCPs with high molecular weights (up to 303000) by copper(I)-catalyzed polymer analogous click reaction (Scheme 1, the right side). A model system was chosen here to show the proof-of-principle, where a series of azo compounds with an azido end group and different flexible spacers were successfully attached onto a polymer with pendant acetylene groups (i.e., poly(propargyl methacrylate), poly(PgMA)), leading to azo-containing side-chain LCPs with high functionalization efficiencies (≥97%). As far as we know, this is also the first report on the synthesis of azo-containing side-chain LCPs with a triazole ring between the polymer backbone and the azo mesogenic moiety. Their chemical structures, phase transition behaviors, and UV/visible light-induced photoisomerization in solutions were studied in detail, and they were also compared with those of the corresponding low molecular weight azo polymers with same structures prepared via the conventional free radical polymerization of the methacrylate azo monomers (prepared via click chemsitry).
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| Scheme 1 The synthetic route to the azo polymers Pn-C and Pn-F (n = 4, 6, 10) by copper(I)-catalyzed polymer analogous click chemistry (the right side) and conventional free radical polymerization (the left side), respectively. | ||
CH–N–), 7.05–6.98 (d, J = 9.2 Hz, 2H, Ar–H), 6.14 (s, 1H, CH
C–), 5.58 (s, 1H, CH
C–), 5.30 (s, 2H, –COOCH2–), 4.43–4.34 (t, J = 7.2 Hz, 2H, –CH2O–Ar–), 4.09–4.02 (t, J = 6.4 Hz, 2H, –NCH2–) and 2.03–1.37 (m, 11H, –(CH2)4–, –CH3).
CH–N–), 7.05–6.97 (d, J = 9.2 Hz, 2H, Ar–H), 6.14 (s, 1H, CH
C–). 5.59 (s, 1H, CH
C–), 5.31 (s, 2H, –COOCH2–), 4.51–4.44 (t, J = 7.0 Hz, 2H, –CH2O–Ar–), 4.14–4.07 (t, J = 6.0 Hz, 2H, –NCH2–) and 2.23–1.84 (m, 7H, –CH2CH2–, –CH3).
C–), 5.58 (s, 1H, CH
C–), 5.30 (s, 2H, –COOCH2–), 4.37–4.30 (t, J = 7.2 Hz, 2H, –CH2O–Ar–), 4.10–4.03 (t, J = 6.4 Hz, 2H, –NCH2–) and 1.97–1.26 (m, 19H, –(CH2)8–, –CH3).
The polymerization of M4 and M10 was performed similarly as for M6, respectively, leading to their corresponding homopolymers (i.e., P4-F and P10-F) in a yield of 70 and 74%, respectively.
The polymer analogous click reaction between poly(PgMA) and N4 or between poly(PgMA) and N10 was performed similarly following the above procedure, leading to the corresponding functionalized polymers (i.e., P4-C and P10-C) in a yield of 93 and 91%, respectively.
Poly(PgMA) was firstly prepared via the conventional free radical polymerization of PgMA in dixoane at 65 °C following a literature procedure,44 but with a much shorter polymerization time. It is known that the free radical polymerization of PgMA is rather difficult to control due to the presence of the reactive acetylene groups, which usually leads to crosslinked polymer networks.45 Therefore, the polymerization condition should be carefully controlled to avoid the occurrence of the possible crosslinking. A poly(PgMA) with a Mn,SEC = 69000 and PDI = 2.10 was readily obtained by using a very short reaction time (45 min) (Table 1, Fig. S1 in the ESI†), which proved to be soluble in common organic solvents such as chloroform, THF, and DMF. The obtained poly(PgMA) was characterized with both 1H NMR (Fig. 1a) and FT-IR (Fig. 2d). The presence of both the proton signal around 2.51 ppm in its 1H NMR spectrum and the absorption peaks around 2129 and 3292 cm−1 in its FT-IR spectrum confirmed the existence of acetylene groups in the polymer. Furthermore, the chemical shifts and the peak integrations of all the protons in the polymer were well consistent with its expected structure.
| Sample | M n,SEC (×10−4) | PDIa | UV absorb. (AU) b | f (%) | M n,UV-vis (×10−5) | Thermal transitioneT/°C | △Hi/J g−1 |
|---|---|---|---|---|---|---|---|
| a The number-average molecular weights (Mn,SEC) and polydispersity indices (PDI) of the polymers determined by SEC with THF (for poly(PgMA), P4-F, P6-F, and P10-F) or DMF containing 0.5 wt% LiBr (for P4-C and P6-C) as the eluent and PS standards. b UV absorbance (at 380 nm, the average values of three measurements) of the azo polymer solutions in DMF (for P4-F, P6-F, P4-C, and P6-C) or in N-methyl pyrrolidone (for P10-F and P10-C) (Cpolymer = 5 × 10−5 mol L−1 azo mesogen). c f refers to the azo functionalization degrees of the polymers, and the f values of the azo polymers Pn-C (prepared via polymer analogous click reaction) were determined by comparing their UV-vis absorbance with that of their low molecular weight counterparts Pn-F. d The number-average molecular weights of the azo polymers Pn-C determined by UV-vis. e G, glassy; SC, smectic C; I, isotropic. f Determined with DSC at the second heating scan under nitrogen (10 °C min−1). g Determined with DSC at the first cooling scan under nitrogen (−10 °C min−1). h No Tg was detectable. i △H represents the enthalpy of the phase transition. | |||||||
| Poly(PgMA) | 6.90 | 2.10 | 0 | ||||
| P4-F | 3.21 | 2.07 | 1.18 | 100 | G 100 f | ||
| G 89 g | |||||||
| P6-F | 2.51 | 2.02 | 1.23 | 100 | G-SC 120 I fh | 3.4 | |
| I 109 SC-G gh | −3.4 | ||||||
| P10-F | 2.77 | 1.90 | 1.21 | 100 | G-SC 114 I fh | 3.2 | |
| I 109 SC-G gh | −2.9 | ||||||
| P4-C | 51.30 | 1.53 | 1.14 | 97 | 2.53 | G 100 f | |
| G 89 g | |||||||
| P6-C | 52.50 | 1.53 | 1.19 | 97 | 2.68 | G 80 f | |
| G 71g | |||||||
| P10-C | 1.20 | 99 | 3.03 | G-SC 125 I fh | 3.8 | ||
| I 119 SC-G gh | −3.2 |
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| Fig. 1 1H NMR spectra of poly(PgMA) in CDCl3 (a), P6-C in DMF-d7 (b), P6-F in CDCl3 (c), and M6 in CDCl3 (d). The peaks from the solvents and water are marked with symbol * and #, respectively. | ||
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| Fig. 2 FT-IR spectra of P4-C (a), P6-C (b), P10-C (c), and poly(PgMA) (d). | ||
A series of azo compounds with an azido end group and different flexible spacers (Nn, n = 4, 6, 10, Scheme 1) were also readily prepared by reacting 1-bromo-n-(4-nitroazobenzene-4′-oxy)alkanes (Bn, n = 4, 6, 10) with an excessive amount of sodium azide. All of them could be obtained in quite good yields, and their purity was satisfactory, as revealed by the thin layer chromatography and 1H NMR techniques.
In the next step, different reaction parameters including the utilized solvent, copper catalyst, reaction temperature, and reaction time were explored in order to provide the optimal reaction conditions for the polymer analogous click reaction. It is known that CuBr/N-alkyl-2-pyridylmethanimine is a highly versatile catalyst for atom transfer radical polymerization.43,46 Recently, it has also proven to be an efficient catalyst for the Huisgen-type cycloadditions.47 Herein, we further checked whether this copper catalyst was also an active catalyst for our study. A model click reaction system between PgMA and Nn (n = 4, 6, 10) was chosen for this purpose (Scheme 1). A series of triazole-containing methacrylate azo monomers (Mn, n = 4, 6, 10) were readily obtained in high yields by performing the reactions in DMF at 60 °C for 12 h with CuBr/NHPMI as the catalyst in the presence of an excess of PgMA. Fig. 1d shows the 1H NMR spectrum of one representative triazole-containing methacrylate azo monomer M6, and the presence of only a single peak at 7.62 ppm for the chemical shift of the triazole ring proton reveals the exclusive formation of the 1,4-disubstituted adduct.
With the starting materials (i.e., poly(PgMA) and Nn (n = 4, 6, 10)) and the optimal click reaction conditions in hand, we tried to perform the polymer analogous click chemistry between poly(PgMA) and Nn (n = 4, 6, 10) (Scheme 1, the right side). The reactions were carried out in DMF at 60 °C in the presence of an excess of Nn with CuBr/NHPMI as the catalyst. The reaction time was extended to 24 h in order to assure a higher functionalization efficiency because a much larger volume of DMF was used in these cases in order to dissolve poly(PgMA) and polymer analogous reactions normally proceed more slowly than the reactions between small molecules. After the coupling reactions, the excess Nn was completely removed from the obtained polymers by washing them with warm methanol, as confirmed with thin layer chromatography. The polymers obtained via the click coupling reactions between poly(PgMA) and Nn (n = 4, 6) (i.e., P4-C, P6-C) were proven to be fully soluble in DMF, while that prepared via the click reaction between poly(PgMA) and N10 (i.e., P10-C) turned out to be only partially soluble in DMF (but it was found to be easily soluble in N-methyl pyrrolidone). The obtained polymers were characterized with FT-IR and 1H NMR. The efficient occurrence of click reactions was demonstrated by the disappearance of the specific IR bands for acetylene groups at 2129 and 3292 cm−1 and the appearance of some new absorption bands associated with the asymmetric (1341 cm−1) and symmetric (1520 cm−1) stretching vibrations of the nitro groups and the ring-stretching mode of the phenyl groups (around 1600 cm−1) (Fig. 2). The 1H NMR spectrum of one representative azo polymer P6-C in deuterated DMF is shown in Fig. 1b, and the chemical shifts and the peak integrations of all the protons in the polymer are in good agreement with its expected structure.
The obtained polymers Pn-F (n = 4, 6, 10) were proved to be soluble in common organic solvents such as chloroform, THF, and DMF. Their number-average molecular weights determined by SEC (Mn,SEC) were found to range from 25100 to 32100 and their PDI were around 2 (Table 1), which are reasonable for the azo polymers prepared via conventional free radical polymerization. Fig. 1c shows the 1H NMR spectrum of one representative azo polymer P6-F in deuterated chloroform, which agrees well with its chemical structure. In addition, it can be seen clearly that the 1H NMR spectrum of P6-F is quite similar with that of P6-C although they were determined in different deuterated solvents, further indicating that the obtained P6-C indeed has the desired chemical structure.
N– bond, respectively.48 By comparing their UV absorption at 380 nm (i.e., AP6-C,380nm and AP6-F,380nm), an azo functionalization degree (f) of 97% was determined for P6-C by using the equation f = (AP6-C,380nm/AP6-F,380nm)×100% (Table 1). It is important to point out here that this approach is facile and efficient for the determination of azo functionalization degrees of the azo polymers because there exists very good linear relationship between the UV absorbance of the azo polymers and their concentrations, even in the cases of rather high concentrations of the azo chromophores (Fig. S2 in the ESI†). Similarly, an azo functionalization degree of 97 and 99% was also obtained for P4-C and P10-C, respectively. These results strongly demonstrated that the copper(I)-catalyzed polymer analogous click reactions between poly(PgMA) and Nn (n = 4, 6, 10) were highly efficient under the studied reaction conditions.
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Fig. 3 UV-vis spectra of the P6-F solution ( ) and P6-C solution ( ) in DMF (CP6-F = CP6-C = 0.025 mg mL−1 = 5.0 × 10−5 mol L−1 azo mesogens). | ||
On the basis of the above-obtained azo functionalization degrees for Pn-C (n = 4, 6, 10) and the molecular weight of poly(PgMA) (Mn,poly(PgMA), which is assumed to be equal to Mn,SEC,poly(PgMA), i.e., 69000), the number-average molecular weights of Pn-C determined by UV-vis (i.e., Mn,UV-vis) can be readily derived by using the following equation:
| Mn,UV-vis = Mn,SEC,poly(PgMA) + x × f × MNn |
P4-C and P6-C were also characterized with SEC by using DMF containing 0.5 wt% LiBr as the eluent. The results showed that P4-C and P6-C had a Mn,SEC of 513000 and 525000, respectively, and both of their PDI were 1.53 (Table 1 and Fig. S3 in the ESI†). The difference between the Mn,SEC and Mn,UV-vis values of the azo polymers might be assigned to the calibration of the SEC on the basis of polystyrene standards.
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| Fig. 4 DSC curves of the azo polymers Pn-C (n = 4, 6, 10) from the first cooling scan (a) and from the second heating scan (b) (±10 °C min−1). | ||
POM study showed that when P10-C was cooled from its isotropic state, a large number of anisotropic entities appeared from the dark background of the isotropic liquid. However, it was impossible to observe any characteristic liquid crystalline texture although the sample was annealed in its liquid crystalline phase for a rather long time (Fig. 5a), probably due to the high polymer viscosity. It has been well-established that the high viscosity of the polymer melts can hinder the formation of well-defined liquid crystalline textures.49 This is especially true for smectic liquid crystalline polymers where the development of two-dimensional positional order promotes a further increase in viscosity.50,51 Nevertheless, the phase transition of P10-C proved to be fully reversible. Its birefringence disappeared completely at 130 °C upon heating (10 °C min−1), and it appeared again at 125 °C upon cooling from the isotropic state at a rate of 10 °C min−1, which suggested that the transition peaks in the DSC curves of P10-C represented the transition between the liquid crystalline phase and isotropic phase and the mesomorphism was enantiotropic. The liquid crystalline textures of the polymer were similar for both the heating and cooling scans (the exact nature of the liquid crystalline phase of P10-C was assigned with the aid of SAXS, as shown in the following part). In contrast to P10-C, no obvious birefringence was observed for both P6-C and P4-C, which is likely to be due to their relatively shorter spacers, thus limiting the decoupling effects between the pendant mesogens and the polymer backbones.52
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| Fig. 5 The POM images upon cooling from the isotropic phases: P10-C at 118 °C (annealed for 70 min) (a), P10-F at 108 °C (annealed for 60 min) (b), and P6-F at 108 °C (annealed for 60 min) (c). | ||
The phase transition behaviors of Pn-C were also compared with those of Pn-F to study the influence of the largely different molecular weights. As shown in Fig. 6, the DSC curves of both P10-F and P6-F exhibited one phase transition peak in both the second heating and the first cooling scans, while there existed no transition peak in those of P4-F. In addition, a glass transition at 100 and 89 °C was observed for P4-F in the DSC second heating and the first cooling scan, respectively, whereas no obvious glass transition was detected for P6-F and P10-F. Note that the Tg value of P4-F is almost the same as that of P4-C although their molecular weights are considerably different, which suggests that the Tg of the studied azo polymers have reached their maximum values at the molecular weights of the low molecular weight polymers and they become leveled off with the further increase in the molecular weights. Similar phenomenon was also reported for other polymer systems previously.53 In contrast, the molecular weights showed much influence on the phase transition temperatures (Ti) of the azo polymers with a flexible spacer =(CH2)10. The Ti value of P10-F was found to be about 10 °C lower than that of P10-C in both the second heating and the first cooling scans (±10 °C min−1) (Table 1), which confirmed the high molecular weight of P10-C and demonstrated that P10-C had a broader liquid crystalline temperature range than its low molecular weight counterpart P10-F.
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| Fig. 6 DSC curves of the azo polymers Pn-F (n = 4, 6, 10) from the first cooling scan (a) and from the second heating scan (b) (±10 °C min−1). | ||
POM observation showed that there existed obvious liquid crystalline textures in both the heating and cooling processes of P10-F and P6-F (Fig. 5b,c). The phase transition peaks in their DSC curves were proven to represent the transition between the liquid crystalline phases and isotropic phases and the mesomorphism was enantiotropic. Similar to P10-C, no well-defined liquid crystalline texture was obtained for P10-F. On the contrary, P6-F showed a batonnet texture of the smectic C mesophase after careful annealing of the sample in its liquid crystalline phase.51 In contrast to P6-F and P10-F, no obvious birefringence was observed for P4-F, which is similar as P4-C. In this context, it is worth mentioning that the presence of the liquid crystalline phase in P6-F instead of P6-C is probably due to their largely different molecular weights. The much lower molecular weight of P6-F might significantly reduce its viscosity above its Tg and allow its mesogenic azo groups to move more freely, thus leading to their more ordered self-assembled molecular structures.
It is well known that SAXS can provide useful information concerning molecular arrangement, packing mode of the mesogen, and type of order in the mesophase of a liquid crystalline polymer and it has thus been widely utilized for accurately assigning the exact nature of the liquid crystalline phases.19,54 Therefore, the liquid crystalline mesophases of both P10-C and P10-F were further studied with in situ variable temperature SAXS. Fig. 7 shows the SAXS patterns of P10-C and P10-F, which were obtained at their liquid crystalline temperatures (with a certain time of annealing) upon cooling from the isotropic states. The results showed that both P10-C and P10-F exhibited one scattering peak at q = 2.95 nm−1, suggesting the existence of an ordered smectic lamellar structure with a layer spacing d = 2.13 nm (d = 2π/q, Fig. 8).54 This d value is smaller than the calculated molecular length (l) for the fully extended side-chain liquid crystalline unit of P10-F or P10-C (l = 3.11 nm), revealing a fully interdigitated smectic C structure (i.e., near to 100% overlap of the side-chain units) with a tilted angle of 46.8° relative to the normal of the polymer backbone, as schematically shown in Fig. 8.
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| Fig. 7 SAXS patterns of P10-C at 118 °C with an annealing time of 80 min (scan time: 60 min) (a) and P10-F at 108 °C with an annealing time of 60 min (scan time: 50 min) (b) upon cooling from the isotropic states. | ||
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| Fig. 8 Proposed liquid crystalline structure for P10-C and P10-F. | ||
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| Fig. 9 UV-vis spectral changes in dependence of time for the P6-C solution in DMF (C = 0.025 mg mL−1) at 25 °C upon irradiation with 365 nm light (a) and upon irradiating the polymer solution at the photostationary state with λ > 430 nm visible light (b). | ||
Fig. 9b shows the UV-vis spectral changes of the P6-C solution in DMF with time under irradiation with λ > 430 nm visible light, where the polymer solution had been irradiated with 365 nm UV light for 210 s prior to the visible light irradiation. It can be seen clearly that the polymer solution underwent cis to trans back-isomerization upon visible light irradiation, but the finally recovered absorbance of trans-azobenzene was lower than that before UV irradiation with the recovery of the trans-isomer being 92%. Similar phenomena were also observed previously.19,55,56 Its cause might be that, at the same wavelength where the cis to trans photochemical back-isomerization was performed, there was also a weak absorption from the trans-isomer, which eventually led to an equilibrium with cis to trans and trans to cis isomerizations taking place under the same visible light after most of the cis-isomer returned to the trans-isomer.13 Nevertheless, the photochemical isomerization became completely reversible upon the subsequent cycles of UV and visible light irradiation (Fig. 10).
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| Fig. 10 UV and visible light-induced photoisomerization cycles of the P6-C solution in DMF (C = 0.025 mg mL−1). In each cycle, the polymer solution was irradiated firstly with UV light for 210 s and then with visible light for 120 s, respectively. | ||
The photochemical isomerization of the P6-C solution in DMF was also compared with that of its low molecular weight counterpart P6-F solution. As expected, the P6-F solution in DMF also underwent reversible trans to cis and cis to trans photoisomerization under the irradiation of UV and visible light, respectively (Fig. 11a and b). The time dependence of their relative absorbance (At/A0, where At refers to the absorbance of the polymer solution at 380 nm at time t upon UV or visible light irradiation and A0 the original absorbance of the polymer solution at 380 nm without UV light irradiation) showed that the photoinduced isomerization rate of the P6-F solution was close to that of the P6-C solution under the irradiation of 365 nm UV light (Fig. 12). However, the relative absorbance of the trans-azobenzene in the photostationary state finally reached for the P6-C solution proved to be somehow larger than that of the P6-F solution. Its real cause is not very clear yet at this point and further investigation is ongoing to provide a reasonable explanation for this phenomenon. In comparison, the photochemical back-isomerization processes of the polymer solutions under the irradiation of visible light were more or less the same, suggesting that the molecular weights of the azo polymers had little influence on their visible light-driven back-isomerization processes.
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| Fig. 11 UV-vis spectral changes in dependence of time for the P6-F solution in DMF (C = 0.025 mg mL−1) at 25 °C upon irradiation with 365 nm light (a) and upon irradiating the polymer solution at the photostationary state with λ > 430 nm visible light (b). | ||
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| Fig. 12 Dependence of the relative absorbance (At/A0) on time upon irradiating with 365 nm UV light (filled symbols) or with λ > 430 nm visible light (empty symbols) for the P6-C solution (cycle) and P6-F solution (triangle) in DMF (C = 0.025 mg mL−1) at 25 °C, respectively. | ||
Footnote |
| † Electronic supplementary information (ESI) available: SEC chromatograms of poly(PgMA), P4-C, and P6-C as well as the dependence of the UV absorbance of the solutions of P6-F and P6-C in DMF on their concentrations. See DOI: 10.1039/c0py00138d |
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