Journal of Nanomaterials

Volume 2013 (2013), Article ID 498920, 12 pages

http://dx.doi.org/10.1155/2013/498920

Research Article

Synthesis and Morphological Transformation of Conjugated Amphiphilic Diblock Copolymers in Mixed Solvents

Yang-Yen Yu,1,2,3 Chung-Yi Hsu,¹ and Guo-You Li¹

¹Department of Materials Engineering, Ming Chi University of Technology, 84 Gungjuan Road, Taishan District, New Taipei City 24301, Taiwan

²Center for Thin Film Technologies and Applications, Ming Chi University of Technology, 84 Gungjuan Road, Taishan, New Taipei City 243, Taiwan

³Battery Research Center of Green Energy, Ming Chi University of Technology, 84 Gungjuan Road, Taishan District, New Taipei City 24301, Taiwan

Received 9 November 2012; Accepted 29 December 2012

Academic Editor: Gong Ru Lin

Copyright © 2013 Yang-Yen Yu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

The synthesis, morphological transformation, and photophysical properties of a rod-coil block copolymer, poly[2,7-(9,9-dihexylfluorene)]-block-poly(2-vinylpyridine) (PF-b-P2VP), with P2VP coils of various lengths in a mixed methanol/tetrahydrofuran (MeOH/THF) solvent are reported. Various morphological structures of PF-b-P2VP aggregates, including spheres, short worm-like structures, long cylinders, and large compound micelles (LCMs), were observed after varying the coil length of PF-b-P2VP and the selectivity of mixed solvents. These aggregated structures demonstrated considerable variation with regard to optical absorption, fluorescence, and the PL quantum yield of rod-coil copolymers. The degree of hypsochromic spectral shift was enhanced as the length of P2VP coils and the content of poor solvent increased. This study reveals the influence of coil length and selectivity of solvents on the morphology and the optical characteristics of rod-coil amphiphilic copolymers.

1. Introduction

The self-assembly of amphiphilic block copolymers (ABCs) is considered a promising approach to synthesize nanostructured or hierarchical materials with novel morphological and physical properties for advanced applications in areas such as electronics, optoelectronics, biotechnology, and environmental technology [1–13]. The morphology of amphiphilic block copolymers can be manipulated using different driving forces, including relative block length, block polarity, volume fraction, and temperature [14–16]. Recently, amphiphilic rod-coil diblock copolymers [17, 18] have attracted considerable attention, as they produce novel self-organizing structures in the form of stiff rod-like segments, such as helical [19] and π-conjugation polymers [20–25]. In the past 5 years, a great number of new π-conjugated polymers have been synthesized and used in various biological applications such as sensing and imaging agents. These studies have focused on highly sensitive diagnosis of pathogenic microorganisms and tumor cells and detection of disease-related biomarkers. Beyond sensing, fluorescence imaging in vitro has also been successfully achieved. Besides, these materials have also attracted much attention for biomedical applications, such as monitoring drug delivery and release, gene delivery, drug screening, and anti-microorganism and anticancer therapies [26–28].

Rod-coil block copolymers containing π-conjugation chains are of particular importance because conjugated homopolymers are among the most promising candidates for low-cost, large-area, flexible organic electronics [29]. The high immiscibility and stiffness asymmetry between rigid conjugated rods and flexible coil segments significantly influence the molecular packing of polymers, leading to self-organized aggregation. The aggregation of rod-like conjugated chains enables the production of a wide variety of supramolecular structures at nanoscale dimensions, including lamellar, spherical, cylindrical, vesicular, and worm-like structures that further influence electronic and photophysical properties [17, 18]. Polyfluorene (PF) and its derivatives have been widely used for polymer light-emitting diodes, owing to their high fluorescence quantum yield and good charge transport ability [30–33]. Although PF is a promising material for light-emitting diodes, PF chains tend to stack cofacially and form excimers due to intermolecular π-π interaction, which results in nonradiative decay and a subsequent reduction in the performance of devices. A diblock architecture is one possible solution to lower the intermolecular interaction in PF and suppress the formation of excimers [34]. Moreover, the photophysical properties are possibly influenced strongly by variations in the morphology of rod-coil copolymers. Rod-coil block copolymers with fluorene-based segments have been reported by several groups [35–37]. The importance of the morphological transformation of rod-coil poly[2,7-(9,9-dihexylfluorene)]-block-poly(2-vinylpyridine) (PF-b-P2VP) via selective solvents on optical characteristics has been demonstrated [22]. Diverse morphological and optical properties can be induced in the aggregate by changing the MeOH/THF ratio. However, the means by which the length of coil segments and solvent quality influence the morphology of PF-b-P2VP have not yet been fully explored.

This study demonstrates the synthesis, morphology, and photophysical properties of amphiphilic PFm-b-P2VPn at a fixed rod length with three different coil lengths (). The chemical structure of the studied polymers and the synthetic scheme for the PF-b-P2VP block copolymer are shown in Scheme 1. By varying the selectivity of the solvents and the annealing temperature, polymers with various aggregation morphologies were induced. This paper reveals the influence of the ratio of poor/good solvents on the morphological and photophysical properties of these di-block copolymers with various coil lengths as well as the spectral stability of PF-b-P2VP. Finally, transmission electron microscopy (TEM), atomic force microscopy (AFM), UV-vis optical absorption, and photoluminescence (PL) spectroscopy were employed to investigate the correlation between optical characterization and morphology.

Scheme 1: Chemical structures of the synthesized PF-b-P2VP rod-coil diblock copolymers.

2. Experimental

2.1. Materials

9,9-dihexyl-2-7-dibromofluorene (F, Aldrich, 97%), 2-Vinylpyridine (2VP, Acros, 97%), copper(I) bromide (CuBr, Aldrich, 99.999%), anhydrous tetrahydrofuran (THF, Echo), N,N,N′,N′,N′′-pentamethyldiethylenetriamine (PMDETA, Aldrich, 99%), anhydrous methyl alcohol (MeOH, Mallinckrodt), n-hexane (Tedia, 95%), Aluminium oxide (50–200 micron, Acros), and chloroform-d (99.8 atm% D, Aldrich) were used as received to prepare the PF-b-P2VP copolymers.

2.2. Synthesis of PF-b-P2VP Copolymers and Preparation of PF-b-P2VP Aggregates in Mixed Solvents

First, α-(4-hydroxymethyl phenyl)-ω-bromo-poly[2,7-(9,9-dihexyl-fluorene)] was synthesized according to the literature [38]. 2-bromo-7-bromohydroxide-9,9-dioctylfluorene was prepared by boronation of 9,9-dihexyl-2,7-dibromofluorene with tri-isopropyl borate at −78°C. The polymerization of the prepared product using a modified Suzuki coupling protocol followed by end capping with bromobenzene yielded α-bromo-ω-phenyl-poly(9,9-dioctylfluorene). Then, a second Suzuki reaction of α-bromo-ω-phenyl-poly(9,9-dioctylfluorene)with an excess of 4-formylphenylboronic acid, now using the well-known toluene-soda two-phase system, yielded almost quantitatively α-(4-formylphenyl)-ω-(phenyl)-poly(2,7-(9,9-dioctylfluorene)). It was then reacted with 2-bromoisobutyl bromide to obtain the polyfluorene macroinitiator, α-{4-[2-(2-bromo-2-methylpropoyloxy)methyl]phenyl}-ω-bromo-poly[2,7-(9,9-dihexyl-fluorene)] (PF-Br). GPC analysis revealed an Mn of 5300 g/mol, which corresponds to ten fluorene repeating units. Finally, poly [2,7-(9,9-dihexylfluorene)]-block-poly(2-Vinylpyridine) (PF-b-P2VP) was synthesized from PF-Br by atom transfer radical polymerization. Taking PF₁₀-b-P2VP₇₅ as an example, 300 mg (1 mmol) of PF-Br, 13.4 mg of CuBr (2 mmol), and 1.056 mL of 2-VP (200 mmol) were added to a dry round-bottom flask, and the system was maintained under vacuum for 30 min. 0.02 mL solution of PMDETA (2 mmol) in 2.6 mL of THF was added into the round-bottom flask under a nitrogen atmosphere. The mixture was degassed three times, filled with nitrogen, stirred at ambient temperature for 30 min, and immersed into an oil bath at 120°C for 24 h. After cooling to room temperature, the mixture was passed through an Al₂O₃ column to remove the copper catalyst, precipitated into an excess amount of n-Hexane, filtered off, and the remaining product dried under vacuum at 30°C to obtain 100 mg of PF-b-P2VP as a black solid (yields: 95%). ¹H NMR (CDCl₃), P2VP block: δ(ppm) = 8.5–8.0, 7.5–6.0 (4H, pyridine), 3.78 (1H, CH(pyr)-C(O)), 2.3, 1.8 (3H, back-bone). GPC: Mn (PF) = 5300, Mn(P2VP) = 10700, PDI = 1.33 for PF₁₀-b-P2VP₃₅; Mn(PF) = 5300, Mn(P2VP) = 11198, PDI = 1.41 for PF₁₀-b-P2VP₅₅; Mn(PF) = 5300, Mn(P2VP) = 14900, PDI = 1.26 for PF₁₀-b-P2VP₇₅. Moreover, the prepared PF-b-P2VP copolymer solid was dissolved into the mixed MeOH/THF solvents with different volume ratios of MeOH/THF, that is, 0, 10, 25, 50, 75, and 90%. During the experiment, it was found that the block chain length of copolymers dominated the morphologies of copolymer aggregates under a fixed copolymer concentration. The effect of polymer concentration could be neglected. Therefore, the polymer concentration of all solution was maintained at 0.1 wt%.

2.3. Characterization

¹H-NMR spectra of the prepared polymers were performed by a Jeol EX-400 spectrometer. The molecular weight was determined using a GPC instrument equipped with a refractive index detector (Schambeck SFD GmbH, model RI 2000), a Lab Alliance solvent delivery system, and a GPC column (PLgel 5 μm mixed, C and D). Calibration was achieved by injecting polystyrene standard diluted to 0.5 wt% in THF (1 mL/min) at 40°C. Thermal analyses were carried out on a differential scanning calorimetry (DSC) from TA instruments (TA Q20) with a heating cycle from room temperature to 200°C at a heating rate of 20°C/min and a thermal gravimetric analyzer (TGA) from TA instruments (TA Q50) with a heating range from room temperature to 900°C at a heating rate of 20°C/min.

The PF-b-P2VP aggregate morphologies were characterized by transmission electron microscopy (TEM) using a JEOL 1210 operating at an acceleration voltage of 100 kV. A drop of the aggregate dispersion was cast onto a 200 mesh copper TEM grid deposited with carbon and dried under vacuum before imaging. The deuterated solvent used for obtaining the spectra was chloroform-d. The AFM data was performed in tapping mode on a Nanoscope DI III multimode AFM. The UV-vis spectra were obtained from polymer thin films prepared on glass by spin coating at a speed of about 1000 rpm using a Jasco Model V-650 spectrometer. The PL spectra were obtained using a Horiba Jobin Yvon Fluoromax-4 Spectrofluorometer with a 450 nm excitation wavelength.

3. Results and Discussion

3.1. Micellar Morphologies

In this study, transmission electron microscopy (TEM) and atomic force microscopy (AFM) are utilized for a more detailed investigation of the morphologies for PF-b-P2VP copolymer in solutions and films, respectively, although dynamic light scattering (DLS) has been applied in the investigation of micellar morphology. However, it is known that DLS is not the appropriate tool to use for gaining deeper information on the morphology of micelles [39]. It is because the analytical result of DLS is obviously affected by the operating condition and calculation method. Besides, DLS cannot provide the real morphologies of micellar aggregation. The selectivity of solvents can be manipulated by selecting solvents with various solubility parameters. The solubility of PF and P2VP is in the range of 18.62–19.02 MPa0.5 and 27.6 MPa0.5, respectively. The solubility of THF and MeOH is 18.6 and 29.7 MPa0.5, respectively. Thus, THF is a suitable solvent for PF and a selective solvent for P2VP. By contrast, methanol is a suitable solvent for P2VP and a selective solvent for PF. Figures 1(a)–1(d) indicate the aggregation behavior of amphiphilic PF₁₀-b-P2VP₃₅ in a mixed solution of MeOH/THF with various methanol contents: 0, 25, 50, and 75 vol.%. Spherical micelles with a diameter ranging from 50–80 nm were observed in pure THF solution. This is because THF acts as a good solvent for PF, but as a poor solvent for P2VP, resulting in a spherical morphology with a core of P2VP and a corona of PF. By increasing the methanol content to 10 vol.%, some of the spherical micelles began aggregating with one another to form short worm-like structures less than 500 nm in length. Increasing the MeOH content to 25 vol.% resulted in short worm-like structures aggregating to form long three-dimensional network structures, several micrometers in length, due to the ability of these structures to efficiently reduce the interfacial energy of the P2VP core and the PF corona [21]. A further increase in the MeOH content to 50 vol.% resulted in the formation of two morphological structures of PF-b-P2VP aggregate: a spherical micelle with a core of PF and a corona of P2VP and a cylinder with a diameter of 50–100 nm and a length of approximately 300–500 nm. This transformation was due to the expansion of the P2VP core following an increase in MeOH, because MeOH is a good solvent for P2VP, and the increased selectivity enhances the π-π stacking of the PF segment, resulting in a cylindrical morphology [22]. When the MeOH content exceeded 75 vol.%, all aggregates of PF-b-P2VP formed spherical micelles with a core of PF and a corona of P2VP, because the mixed solution containing a large proportion of MeOH facilitated the stretching of hydrophilic P2VP and the aggregation of the hydrophobic PF. Thus, the P2VP core and PF corona prefer to invert to a PF core and P2VP corona in the presence of large quantities of MeOH [21]. The diameter of the phase-inversed spherical aggregate comprising a PF core and P2VP corona was in the range of 50–80 nm. When the ratio of MeOH/THF increased to 90 vol.%, further aggregation between the small micelles occurred to produce larger spherical aggregates up to 200 nm in diameter, exceeding the size of aggregates comprising a P2VP core and PF corona. This increase in the size of micelles results from the P2VP chain being longer than the PF chain. Figures 1(e) and 1(f) show AFM images of the topography of PF₁₀-P2VP₃₅ thin films prepared from mixed solutions of MeOH/THF with 25 vol.% and 50 vol.% MeOH, respectively. The images also illustrate the morphologies described previously, in agreement with those obtained from TEM.

(a)

(b)

(c)

(d)

(e)

(f)

Figure 1: TEM images of (PF)₁₀-b-(P2VP)₃₅ aggregates in dilute solution of MeOH/THF with methanol contents of (a) 0, (b) 25, (c) 50, and (d) 75 vol.%. (e) and(f) show the AFM images for the thin films of PF₁₀-P2VP₃₅ prepared at 25 and 50 vol.% MeOH content, respectively.

As the length of hydrophilic P2VP coils increased from 35–55 nm, a similar morphological transformation was observed. Figures 2(a)–2(d) show TEM images of PF₁₀-b-P2VP₅₅ in a mixed solution of MeOH/THF. Aggregates of PF₁₀-b-P2VP₅₅ exhibited spherical micelles, similar to PF₁₀-b-P2VP₃₅ in pure THF solution. The diameter of the micelles was approximately 70–130 nm, exceeding that of PF₁₀-b-P2VP₃₅ owing to the longer P2VP chain. With an increase in MeOH content to 10 vol.%, the size of the micelles increased, due to the stretching of the long P2VP chains. The diameter of PF₁₀-b-P2VP₅₅ ranged from 100–150 nm. Although the PF chains shrank with an increase in MeOH content, P2VP possesses a longer chain than PF; therefore, the volume of P2VP chains increased more than that of PF chains. Although the MeOH content increased to 25 vol.%, large compound micelles (LCMs) with a diameter of 300–500 nm were observed. The formation of LCMs probably arises from the interpenetration of PF into P2VP. An increase in the MeOH content to 50% resulted in the occurrence of phase-inverted micelles with a PF core and P2VP corona, the diameter of which was 50–80 nm. A worm-like morphology was observed with MeOH contents of 75 and 90 vol.% because the aggregation of worm-like micelles reduces the stretching of P2VP, leading to a decreased entropy loss [22]. Figures 2(e) and 2(f) show AFM images of the topography of PF₁₀-P2VP₅₅ thin films prepared from mixed solutions of MeOH/THF with 25 and 50 vol.% MeOH, respectively. The images exhibit the morphologies described by the TEM analysis.

(a)

(b)

(c)

(d)

(e)

(f)

Figure 2: TEM images of (PF)₁₀-b-(P2VP)₅₅ aggregates in dilute solution of MeOH/THF with methanol contents of (a) 0, (b) 25, (c) 50, and (d) 75 vol.%. (e) and(f) show the AFM images for the thin films of PF₁₀-P2VP₅₅ prepared at 25 and 50 vol.% MeOH content, respectively.

Figures 3(a)–3(d) show TEM images of PF₁₀-b-P2VP₇₅ in mixed solvents of MeOH/THF, in which the longer P2VP chains in PF₁₀-b-P2VP₇₅ provide a stronger driving force to form a long cylindrical morphology, leading to the coexistence of spherical and short worm-like micelle aggregates in the pure THF solution. The diameters of the spherical and worm-like micelles were 120–180 nm and 180–250 nm, respectively. With an increase in MeOH content to 10 vol.% and 25 vol.%, the size of the worm-like micelles extended to several micrometers. Increasing the MeOH content to 50 vol.% resulted in the transformation of the worm-like structures into long cylindrical structures with phase-inverted micelles comprising a PF core and P2VP corona. The length of the cylindrical structures was about several to ten micrometers. As the methanol content was increased to 75 vol.%; all aggregates of PF-b-P2VP formed phase-inverted spherical micelles with a core of PF, a corona of P2VP, and a diameter of approximately 100–150 nm. With a methanol content of 90 vol.%, the swelling of P2VP increased, due to an increase in the solubility of P2VP, resulting in well-dispersed spherical micelles, which increased in size from 150–250 nm. Figures 3(e) and 3(f) show AFM images of the topography of PF₁₀-P2VP₅₅ thin films prepared from mixed solutions of MeOH/THF with MeOH content of 50 vol.% and 75 vol.%, respectively. The images also exhibit the long cylindrical and spherical aggregates described previously.

(a)

(b)

(c)

(d)

(e)

(f)

Figure 3: TEM images of (PF)₁₀-b-(P2VP)₇₅ aggregates in dilute solution of MeOH/THF with methanol contents of (a) 0,(b) 25,(c) 50, and (d) 75 vol.%. (e) and (f) show the AFM images for the thin films of PF₁₀-P2VP₇₅ prepared at 50 and 75 vol.% MeOH content, respectively.

3.2. Photophysical Properties

Figure 4 shows the optical absorption and photoluminescence (PL) spectra of PF₁₀-P2VP₇₅ in a dilute solution of MeOH/THF with MeOH content ranging from 0 to 90 vol.%. The photophysical properties of PF₁₀-P2VP₃₅, PF₁₀-P2VP₅₅, and PF₁₀-P2VP₇₅ are summarized in Table 1. Photophysical analysis shows that both the maximum absorption and photoluminescence spectra of PF₁₀-P2VP₃₅, PF₁₀-P2VP₅₅, and PF₁₀-P2VP₇₅ thin films exhibit a hypsochromic shift with an increase in MeOH from 0–90 vol.%. The hypsochromic shift is probably due to the fact that the aggregation induced by the poor solvent results in PF segments of reduced coplanarity, leading to a reduction in effective conjugation length [21]. In general, the hypsochromic shift of the absorption spectra is attributed to H-type aggregation, in which conjugation segments are oriented in a parallel direction [22], as shown in Scheme 2. H-type aggregation leads to a blue shift in the absorption spectra and a quenching of fluorescence. The maximum UV-vis peaks of PF₁₀-P2VP₃₅, PF₁₀-P2VP₅₅, and PF₁₀-P2VP₇₅ shifted from 374 nm in pure THF solvent to 362, 362, and 356 nm, respectively, in 90 vol.% MeOH. A similar hypsochromic shift was observed in the PL spectra of PF₁₀-P2VP75 with two emission peaks attributed to the radiative decay of singlet excitons. The maximum PL peaks of PF₁₀-P2VP₃₅, PF₁₀-P2VP₅₅, and PF₁₀-P2VP₇₅ shifted from 416 nm, 416 nm, and 415 nm in pure THF solution to 412, 410, and 408 nm, respectively, in 90 vol.% MeOH. Moreover, the PL quantum yields of PF₁₀-P2VP₃₅, PF₁₀-P2VP₅₅, and PF₁₀-P2VP₇₅ decreased from 75, 72, and 71% in pure THF solution to 55, 55, and 45%, respectively, in 90 vol.% MeOH. The degree of hypsochromic shift and the decrease in PL quantum yield increased as the length of P2VP coils and the content of the poor solvent increased, indicating that photophysical properties can be manipulated by the coil length of the P2VP block and the selectivity of the solvents.

Table 1: UV-vis and PL characteristics of PF₁₀-b-P2VP₃₅, PF₁₀-b-P2VP₅₅, and PF₁₀-b-P2VP₇₅ thin films in the various ratios of MeOH/THF solvents.

MeOH/THF¹
PF₁₀-b-P2VP₃₅
PF₁₀-b-P2VP₅₅
PF₁₀-b-P2VP₇₅

(nm)
(nm)
(%)
(nm)
(nm)
(%)
(nm)
(nm)
(%)

0/100
374
416
75
374
416
72
374
415
71

10/90
374
416
68
374
416
65
374
414
64

25/75
374
415
60
372
416
58
374
415
56

50/50
372
414
59
372
415
56
370
413
52

75/25
366
413
57
366
412
55
364
411
48

90/10
362
412
55
362
410
55
356
408
45

The various volume ratios of MeOH/THF solvent.

The maximum peaks of UV-vis spectra.

The maximum peaks of PL spectra.

The quantum yields of PL.

Scheme 2: Schematic illustration of (a) H-type and (b) J-type aggregates of diblock PF-b-P2VP copolymers.

Figure 4: Optical absorption and photoluminescence spectra of (PF)₁₀-b-(P2VP)₇₅ in dilute solution of THF and methanol with methanol contents ranging from 0 to 90 vol.%.

3.3. Effects of Thermal Annealing on Morphology and Photoluminescence

The thermal properties of polymers examined by TGA and DSC are shown in Figure 5. In the inset of Figure 5, the thermal degradation temperature (weight loss of 5%) of (a) PF-vinyl macroinitiator, (b) pure P2VP, (c) PF₁₀-b-P2VP₃₅, (d) PF₁₀-b-P2VP₅₅, and (e) PF₁₀-b-P2VP₇₅ was observed at 394, 360, 367, 363, and 361°C, respectively. The glass transition temperatures of the previously mentioned five polymers were determined from the DSC curves at 86, 109, 112, 109, and 109°C, respectively. The values of and for the prepared di-block copolymers are close to those of the P2VP homopolymer, because the molecular weight of the P2VP moiety is much greater than that of the PF moiety [22]. Figure 6 shows AFM images of the PF₁₀-P2VP₇₅ thin films annealed at room temperature, 80°C, 160°C, and 240°C. At room temperature, the morphology of PF₁₀-P2VP₇₅ exhibited a rough surface. With an increase in annealing temperature, surface roughness decreased, presumably because the thermal energy facilitated the movement of polymer chains, which smoothed the surface at higher temperatures. Figures 7 and 8 show the PL spectra of macroinitiators PF-Br and PF₁₀-P2VP75, respectively, as a function of annealing time at 120°C. Thin films of PF macroinitiator and PF₁₀-P2VP₇₅ were prepared by spin coating and annealing at 120°C in a convection oven for various durations ranging from 0 to 15 h prior to the measurement of PL. Both samples were heat-treated under the same experimental conditions. The results show that the PL emission of PF-Br and PF₁₀-P2VP₇₅ increases in the range of 500–600 nm with amplified annealing times, indicating the formation of excimers. The emission of PF-Br at 525 nm is much stronger than that of PF₁₀-P2VP₇₅, which means that PF₁₀-P2VP₇₅ possesses better spectral stability at higher temperatures. The enhanced stability is probably due to the fact that the P2VP coil suppresses the formation of excimers in the PF blocks during annealing at high temperatures [40].

Figure 5: DSC thermograms of (a) PF-vinyl macroinitiator, (b) pure P2VP, (c) PF₁₀-b-P2VP₃₅, (d) PF₁₀-b-P2VP₅₅, and (e) PF₁₀-b-P2VP₇₅. The inset shows the TGA curves of the previously mentioned corresponding four polymers.

(a)

(b)

(c)

(d)

Figure 6: AFM images of (PF)₁₀-b-(P2VP)₇₅ obtained at various heating temperature of (a) room temperature, (b) 80°C, (c) 160°C, and (d) 240°C, respectively.

Figure 7: Photoluminescence spectra of the thin film of PF macroinitiator annealed at 120°C for 0 h, 1 h, 3 h, 6 h, 9 h, 12 h, and 15 h.

Figure 8: Photoluminescence spectra of the thin film of PF macroinitiator, (PF)₁₀-b-(P2VP)₇₅ annealed at 120°C for 0 h, 1 h, 3 h, 6 h, 9 h, 12 h, and 15 h.

4. Conclusions

The synthesis, morphology, and photophysical characterizations of three amphiphilic rod-coil diblock copolymers comprising PF and P2VP with coil chains of various lengths have been demonstrated. A range of morphologies, including spherical, cylindrical, worm-like, dendritic, and large-compound micelles, were observed by varying the coil length and selectivity of mixed MeOH/THF solvents. These morphologies induce considerable variation in the optical absorption, fluorescence, and PL quantum yields of rod-coil diblock copolymers. The degree of hypsochromic shift and PL quenching are enhanced with an increase in the length of the P2VP coil and the proportion of poor solvent, due to H-type aggregation. This indicates that photophysical properties can be manipulated according to the coil length of the P2VP block and the selectivity of solvents. Furthermore, the P2VP segments efficiently suppress the formation of excimers, indicating that the spectral stability of polyfluorene can be improved through manipulation of the architecture of diblock rod-coil copolymers. This study demonstrates the importance of coil length and the selectivity of solvents on the morphology and optical characteristics of rod-coil copolymers. Further, the importance of rod length on the morphology and optical characteristics of rod-coil copolymers will be investigated in our next study.

Acknowledgment

The authors would like to acknowledge the financial support of the National Science Council through Project NSC 101-2221-E-131-006-MY3.

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