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Hydrogen-Bonded Supramolecular Conjugated Polymer Nanoparticles for White Light-Emitting Devices

Hydrogen-Bonded Supramolecular Conjugated Polymer Nanoparticles for White Light-Emitting Devices
Hydrogen-Bonded Supramolecular Conjugated Polymer Nanoparticles for White Light-Emitting Devices

Communication Macromolecular Rapid Communications https://www.doczj.com/doc/2417790170.html, 895DOI: 10.1002/marc .201300831light-emitting devices (WLEDs) by high-throughout solu-

tion processing, such as roll-to-roll or inkjet printing tech-

niques. [7,8] To achieve the fabrication of such devices, a core issue is to construct optical nano-inks that consist of high-quality and emission color-tunable semiconducting polymer nanoparticles (SPNs) via nano-engineering. [9]

The nanoparticle chemistry of conjugated polymers

affords diverse preparation methods [10–13] and modi? ca-

tion strategies, such as doping, [14]nanocomposites,[15]

encapsulation, [16] or surface modi? cation, [17] to con-trol exciton behavior and energy transfer. [18,19]Gen-erally, white-emitting polymer nanoparticles can be achieved by manipulating ? uorescence resonance energy transfer (FRET) via controlling intraparticle or interpar-ticle doping. [18,20,21] However, with regard to the exten-

sive application of biomedicines, [11,18,22–25]conjugated

poly m er nanoparticles (CPNs) for organic devices, [20,26–29] especially WL EDs, are severely lagging since the pio-neering exploration of polymer light-emitting devices (PL EDs) and polymer solar cells (PSCs) by Scherf and co-workers. [26,27] Fréchet et al. demonstrated a site isolation approach to control the energy transfer of encapsulating nanoparticles for WL EDs. [21] For the blue-emitting prop-erty of poly? uorenes (PFs) nanoparticles, [10,11] Tuncel et al. S upramolecular poly? uorenol enable assembly into conjugated polymer nanoparticles (CPNs). Poly{9-[4-(octyloxy)phenyl]? uoren-9-ol-2,7-diyl} (PPFOH)-based supramolecular nanoparti-cles are prepared via reprecipitation. PPFOH nanoparticles with diameters ranging from 40 to 200 nm are obtained by adding different amounts of water into DMF solution. Size-dependent luminescence is observed in PPFOH-based hydrogen-bonded nanoparticles that is different from that of poly(9,9-dioctyl? uorenes). Finally, white light-

emitting devices using CPNs with a size of 80 nm exhibit

white emission with the CIE coordinates (0.31, 0.34).

Amphiphilic conjugated polymer nanoparticles are poten-

tial organic nano-inks for the fabrication of organic devices

in printed electronics.

H ydrogen-Bonded Supramolecular Conjugated Polymer Nanoparticles for White Light-

Emitting Devices

J in-Yi L in ,J enIt W ong ,L ing-Hai X ie ,*X iao-Chen D ong ,H ui Ying Y ang ,*W ei H uang *

D r. J.-Y. Lin, Prof. L.-H. Xie, Prof. W. Huang C enter for M olecular Systems and Organic Devices (CM SOD), Key Laboratory for Organic Electronics & Information Displays (KLOEID) and Institute of Advanced M aterials (IAM ), N anjing University of Posts and Telecommunications, N anjing 210003,P .R.China E-mail:i amlhxie@https://www.doczj.com/doc/2417790170.html,;iamwhuang@https://www.doczj.com/doc/2417790170.html, D r J. Wong, Prof. H. Y. Yang

P illar of Engineering Product Development, S ingapore University of Technology and Design, S ingapore E-mail:y anghuiying@https://www.doczj.com/doc/2417790170.html,.sg P rof. X.-C. Dong, Prof. W. Huang J iangsu-Singapore Joint Research Center for Organic/Bio- Electronics & Information Displays, Institute of Advanced M aterials,N anjing Tech University N anjing 211816,P .R.China

1.I ntrod uction L ow-cost, large-area, and solid-state light sources have attracted much scienti? c and industrial interest in the background of the energy crisis. [1–6] One appealing and potential method is ecofriendly nanoparticle-based white Macromol. Rapid Commun. 2014, 35, 895?900

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J.-Y. Lin et al.

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896demonstrated CPN-based WL EDs with CIE coordinates of (0.28, 0.34) by controlling the photochemical cross-linking

reaction to tune low-band emission at 530–550 nm. [28]In this context, it is signi? cant to explore delicate methods

for white-emitting conjugated polymer nanoparticles. Herein, we constructed hydrogen-bonded supramolecular

conjugated polymer nanoparticles (SCPNs) with size-dependent luminescence for WLEDs. S ize-dependent luminescence is the typical feature in inorganic quantum dot and nanoparticles when the size is smaller than the critical exciton Bohr radius. However, organic or polymer nanoparticles with the feature of the size-dependent emissions have not been observed in the literature systemically. [27,30–33] For example, poly(9,9-

dioctyl? uorene) (PFO) nanoparticles have been obtained via reprecipitation, and demonstrated optical properties similar to bulk ? lm. [30] One reason is that polymer semi-conductors have intrinsic split energy levels. Besides, the

other reason would be the driving force for the formation

of CPNs, namely weaker hydrophobic and π–πstacking

interactions. [10,11] An alternative is to explore size-dependent FRET processes. Supramolecular approaches allow for not only affording robust non-covalent driving forces to make high-quality nanoparticles, but also manipulating exciton and FRET behaviours by subtle arrangement of chain packing during assembled aggre-gation. [34] As a result, supramolecular conjugated poly-mers (SCPs) are an appealing molecular building block for

self-assembling into nanoparticles with stimuli-respon-

sive luminescence changes that have obvious advan-

tages over general conjugated polymers. [35] Herein, we designed a poly{9-[4-(octyloxy)phenyl]? uoren-9-ol-2,7-

diyl} (PPFOH) bearing hydrogen-bonded supramolecular steric carbinols at the 9-position of poly? uorene (PFs) as

a state-of-the-art model of SCPs to demonstrate distin-guished supramolecular assembly and intriguing par-ticle-size dependent behavior. PPFOH

can assemble into high-quality nano-

particles via reprecipitation. Further-

more, its amphiphilic features make

PPFOH aggregate emissions with the

green–yellow color that are combined

with blue light-emitting backbone of

PFs acting as host to compose a perfect

FRET nanosystem. As a result, the size-

dependent emissions of the hydrogen-

bonded SCPNs were observed that offer

an unprecedented alternative strategy

for WLEDs. Devices with the con? gura-

tion of Au/ p -SiC/PPFOH nanoparticles/

ITO exhibited stable and puri? ed white emission with the CIE coordinates of (0.31, 0.34). 2.R esults and Discussion

2.1. S ynthesis and Characterizations of PPFOH and PPFO8

P PFOH, together with controlled poly{9-(octyloxy)-9-[4-(octyloxy) phenyl]? uoren -2,7-diyl} (PPFO8), were prepared

according to our previous work (Scheme 1 a ).

[ 35 ] Gel permea-tion chromatography (GPC) shows that PPFOH has number-average molecular weight (M n ) and polydispersity index

(PDI) of about 5.4 × 10

4 and 1.46, respectively (Figure S1 in the Supporting Information). The control sample PPFO8 had

M n of 6.92 × 10 4 and PDI of 1.62. As showed in Figure S2, the peaks at 3550 and 3450 cm

?1 in the Fourier-transform infrared (FT-IR) spectra of PPFOH powders, involving

hydroxyl groups, suggested both free hydroxyl groups and

association of hydroxyl groups. The solubility of PPFO8 is similar to poly(9,9-dioctyl? uorene) (PFO) that exhibits excel-lent solubility in common organic solvents such as chloro-form (CHCl 3

) and toluene, but extremely poor solubility in N ,N -dimethylformamide (DMF) due to the larger difference of solubility parameters between PPFO8 or PFO (9.5) and

DMF (12.1).

[ 35 ] In contrast, PPFOH exhibited good solubility in DMF that probably contributed to its slightly amphiph-ilic feature and the formation of hydrogen bonds between

hydroxyl groups and DMF molecules. As a result, amphiphilic

PPFOH–DMF complexes are favorable for assembling by the control of external conditions, such as the addition of poor solvent. [ 12,36,37 ] However, the controlled PPFO8 is insoluble in DMF with poor capability of supramolecular assembly.

P reparation of PPFOH Nanoparticles

N anoparticles of PPFOH were achieved by the reprecipita-tion method. Size-controllable nanoparticles were obtained Macromol. Rapid Commun. 2014, 35, 895?900

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2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim S cheme 1. a ) Synthetic routes of PPFOH and PPFO8. b) PPFOH nanoparticles obtained via re-precipitation, together with the photographs of nanoparticle suspensions by expo-sure to UV 365 nm. PPFOH nanoparticles consist of random polymer chains (host) and hydrogen bonded aggregates (guest).

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by adding H 2 O into DMF solution. Colloidal nanoparticle suspensions exhibited a milky white color owing to light scattering compared to pristine colorless DMF solution (Scheme 1 b ). The general PFO nanoparticles were prepared via a two-steps reprecipitation as follows: dilute tetrahy-drofuran (THF) solution was added into poor solvent (H 2O ) and the THF was removed via heating under ultrasonica-tion. The number density of CPNs in the suspension was too low and it could not be spin-coated to obtain high-quality nanoparticle ? lms. [ 10,11 ] In contrast, for PPFOH it was hard to obtain nanoparticles via two-step reprecipi-

tation but rather by direct precipitation under the same

preparation conditions. The sizes of PPFOH nanoparticles can be tuned from 40 to 200 nm by controlling the ratio of DMF:H 2 O . The sizes were determined to be about 200, 120, 80, and 40 nm at ratios of 300:6, 300:10, 300:20, and 300:50, respectively (Figure 1 ). The diameters of these nanoparti-cles were determined by dynamic light scattering (DLS) to be about 600, 170, 100, and 70 nm (Figure S3). In considera-tion of the kinetically frozen processing of reprecipitation, it is reasonable to explain that the diam-

eter of colloidal nanoparticles decreased

with the increasing amount of added

H 2 O owing to the increased number of

nucleic cores. [ 36,38 ] The diameters in the

DL S analysis larger than those obtained

from SEM images can be explained by

the swelling effect of nanoparticles in

dispersion. In constrast, the controlled

PPFO8 could not assemble into nano-

particles via this method. These results

suggest that supramolecular function-

alization by tethering hydroxyl groups

on the polymer backbones affords an

effective approach to improve the capa-

bility of supramolecular assembly of hairy-rod conjugated polymers into size-controllable nanoparticles via the

formation of amphiphilic polymer–sol-

vent complexes. In contrast to PPFOH

powders, for the PPFOH nanoparticles,

only the lower wavenumber at 3400

cm ?1 involving hydroxyl groups was

found in the FT-IR spectra, indicated

that only association of hydroxyl groups

existed in the nanoparticles (Figure S2).

In this context, there existed stronger

hydrogen-bonding interactions in the

nanoparticles than in the powder state,

which would result in stronger energy

transfer. Meanwhile, SEM analysis was

explored to investigate the stability of the nanoparticles in suspension. We

used nanopaticles with a diameter of

80 nm as an example. In Figure S4, the diameter of pristine nanoparticles was about 80 nm. For the nanoparticles suspension with aging of 0.5 h, the diam-eter was about 80 nm, similar to pristine nanoparticles but exhibiting aggregation. With prolonged aging to 2 h, the diameter was maintained at 80 nm but further signi? -cant aggregation was demonstrated. Thus, there was not growth of the nanoparticles in the suspension with pro-longing aging time, but aggregation of nanoparticles was exhibited.

2.2. S teady and Transient Optical Properties of PPFOH Nanoparticles

T he optical properties of PPFOH nanoparticle suspensions were investigated by electronic absorption spectra; the steady-state and transient photoluminescence (PL) spectra are shown in Figure 2 a , S5, S6, S7 and Table S1. PPFOH in DMF solution (< 0.1 mg mL –1 ) has the maximum absorb-ance peak at about 390 nm that is probably attributable to Macromol. Rapid Commun. 2014, 35, 895?900

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2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim F igure 1. S EM images of the PPFOH-based nanoparticles. PPFOH nanoparticle suspen-

sions with the condition of DM F: H 2O =

300:50 (a), 300:20 (b), 300:10 (c) and 300:6 (d). The scale bars represent 200 nm. e) Diameters vs. the amounts of H 2

O . DMF solution: 1 mg mL –1 ,

300 μL. F igure 2. P L spectra and CIE coordinates of PPFOH nanoparticles suspension with dif-

ferent sizes: a) PL spectra, and, b) their CIE coordinates. All dataa were collected with

excitation at 380 nm.

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the main chains of poly? uorene (Figure S5). The PL spectra

of PPFOH in dilute solution have three emission peaks at

419, 443, and 472 nm that were assigned, respectively, to

the 0–0, 0–1, and 0–2 intrachain singlet transitions of the

poly? uorene backbone. [ 39 ] Three emission peaks exhib-

ited a single-exponential ( 1 A *) decay, and their lifetimes were about 400 ps corresponding to three peaks of the poly? uorene ? uorescent spectrum (Table S1). [ 40 ] The emis-

sion spectra of PPFOH nanoparticles exhibited two energy regimes: blue emission at 440–460 nm and green–yellow at 530–540 nm; this was dramatically different from the

pristine PFO nanoparticles prepared via reprecipitation without green–yellow band emission,

[ 41 ] but similar to the nanoparticles of amphiphilic oligo? uorene or poly? u-

orenes, suggested the existence of aggregates.

[ 12,36,37 ]For nanoparticle suspensions obtained via reprecipitation, emission peaks at ca. 460 and 535 nm had lifetimes of ca. 112 ps and 2.92 ns (Figure S6 and Table S1), affording evi-dence for the aggregates rather than ? uorenone, according to previous investigations. [ 42–44 ] These assumptions are supported by the FT-IR spectra in which the feature peak

of ketone at 1720 cm ?1 was not observed (Figure S2). It can

be deduced that the aggregate species, together with the

pristine poly? uorene chains in nanoparticles, consist of a

self-doping energy transfer host–guest nanosystem.

S ize-dependent emissions of PPFOH nanoparticles have been observed in Figure 2 and S7. For nanoparticle

suspensions obtained via reprecipitation, the intensity of green–yellow band emission was increased with the decreased size of nanoparticles (Figure 2 a ). For reprecipi-tation with the frozen process, the intensity of green–yellow band emissions is associated

with the amount of aggregates. This

can be explained by a proportional

relation between the number of nuclei

and the amount of aggregates with

increasing amount of H 2

O . From Figure S7, the intensity of green–yellow emis-

sion of PPFOH nanoparticle ? lms spin-

coated from nanoparticle suspension

also increased with decreasing size of

nanoparticles, and was stronger than

the intensities of the corresponding

nanoparticle suspension. PPFOH nano-

particle suspension and ? lm with diam-

eter of 200 nm exhibited blue emission

with the CIE coordinates (0.17, 0.16) and

near-white emission with CIE coordi-

nates of (0.24, 0.33), respectively. PPFOH

nanoparticle suspensions with size

of 80 nm exhibit white color with CIE coordinates (0.30, 0.42) but slight green color with CIE coordinates (0.29, 0.48). The particle thin ? lms exhibited similar size-dependent photoluminescence with high intensity of green emission with reduced particle size. The intensi-ties of green–yellow emission of nanoparticle ? lms spin-coated from suspension was stronger than those of the corresponding nanoparticle suspensions. Size-dependent photoluminescence offers an alternative ?

exible method to tune emission colors.

2.3.E lectroluminescence Properties of PPFOH Nanoparticle-Based WLEDs

H ybrid WL EDs with the con? guration Au/ p -SiC/PPFOH nanoparticles/ITO were fabricated in order to explore the potential applications of nanoparticles thin-? lm devices (Figure 3 ). According to previous works, [ 45–48 ] the electrolu-minescent (EL) spectra in this kind of hybrid nanostructure-based LED exhibit ineffective energy transfer with respect to the photoluminescence. Therefore, PPFOH colloidal repre-cipitated nanoparticles with size of 80 nm (PL spectral with

CIE coordinates (0.30, 0.42)) were selected to fabricate the

WLEDs, in which nanoparticle thin ? lms were obtained via spin-coating from suspensions on the p -SiC (Figure S8). The current–voltage ( I –V ) curves in the hybrid WL EDs exhib-ited typical rectifying characteristics (Figure 3 b ). When the hybrid WLEDs was forward biased to about 15 V, the current reached up to 2.33 mA, while only a small reverse leakage current of 0.02 mA was observed at ?15 V. The hybrid WLEDs has turn-on voltage (current) of ca. 15 V (2.33 mA).

T he EL spectra of hybrid WL EDs based on the nanopar-ticles at various forward biased voltages are showed in Figure 3 c and no light emission was observed from the Macromol. Rapid Commun. 2014, 35, 895?900

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2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim F igure 3. a ) The device con? guration of the hybrid WLEDs based on PPFOH nanoparticles. b) Current–voltage ( I –V ) curve of the hybrid WLEDs; the inset is the enlarged current–voltage curve at the reverse bias. c) EL spectra at different voltages. d) CIE coordinates of hybrid WLEDs biased at various voltages.

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hybrid WLEDs under reverse bias. The EL spectra of hybrid WL EDs can be ? tted by three Gaussian curves with peak wavelengths at around 433, 474, and 535 nm that were

consistent with the PL pro? les (Figure 3 c ). The EL spectra showed lower emission intensities at long wavelength and

broad emission as compared with the PL spectra. For devices

based on PPFOH nanoparticles, EL spectra have the CIE chromaticity coordinates of (0.28, 0.32), (0.31, 0.34), (0.31, 0.32), and (0.35, 0.36) at 15, 20, 27.5, and 30 V, respectively. These values are well matched with the most optimized white light, with the CIE coordinates (0.33, 0.33) (Figure 3 d ). In addition, it should be noted that the EL spectra of PPFOH thin ? lm spin-coated from DMF solution for comparison exhibited only one emission peak at 560 nm under these experimental conditions. This supports the notion that nanoparticles are favorable for the white emission. 3.C onclusions W e have demonstrated state-of-the-art supramolecular conjugated polymer nanoparticles for application as WLEDs. In comparison with the controlled PPFO8 without hydroxyl group, hydrogen-bonded supramolecular conju-gated polymer PPFOH exhibited excellent supramolecular assembly behavior. PPFOH nanoparticles were obtained with size ranging from 40 to 200 nm via reprecipitation. PPFOH nanoparticles have fascinating size-dependent luminescent properties, affording a ? exible method to tune their emission color from blue–green, yellow to white. PPFOH nanoparticles with size of ca. 80 nm were observed to emit nearly white light with the CIE coordinates (0.30, 0.42). Prototype WL EDs using PPFOH nanoparticles with size of 80 nm exhibited white emission color with the CIE coordinates (0.31, 0.34) at 20 V. Supramolecular conjugated polymers are intriguing and versatile building blocks for self-assembly, and supramolecular polymer nanoparti-cles that will be promising organic nanoinks not only for WLEDs but also for organic nanodevices. S upporting Information S upporting Information is available from the Wiley Online Library or from the author. A cknowledgements: T he project was supported by the National Natural Science Funds for Excellent Young Scholar (21322402), the National Natural Science Foundation of China (21274064, 21144004, 61177029, 20974046), The Program for New Century Excellent Talents in University (NCET-11–0992), the Doctoral Fund of Ministry of Education of China (20133223110007), the Natural Science Foundation of Jiangsu Province (BK2011761, BK2008053, SJ209003), and the Program for Postgraduates Research Innovation in University of Jiangsu Province (CXLX11_0413, CXLX11_0423).[1]E .F.S chubert ,J .K.K im ,S cience 2005,308,1274.

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