Nanlong Hongab,
Xueqing Qiu*ab,
Wanyuan Dengc,
Zhicai He*c and
Yuan Li*ab
aSchool of Chemistry and Chemical Engineering, South China University of Technology, Guangzhou, China. E-mail: celiy@scut.edu.cn
bState Key Laboratory of Pulp and Paper Engineering, South China University of Technology, Guangzhou, China
cInstitute of Polymer Optoelectronic Materials and Devices, State Key Laboratory of Luminescent Materials and Devices, South China University of Technology, Guangzhou, China. E-mail: zhicaihe@scut.edu.cn
First published on 9th October 2015
Using lignosulfonate (LS) and alkyl chain-coupled lignosulfonate-based polymer (ALS) as the raw materials, the aggregation behavior of LS and ALS was investigated, and they both showed a unique aggregation behavior to form a block-like self-assembly for the first time. The aggregation behavior and mechanism of LS and ALS were investigated by SEM, TEM and DLS. The block-like aggregates prepared from ALS (micron size) were larger than that of LS (nano size). The unique aggregates were also further confirmed by XPS, meanwhile, SAXS was applied to explore the regular intrinsic characteristics of the block-like aggregates. Inspired by the aggregation behavior of LS and ALS, the electron transfer properties of LS and ALS were also studied including the electrochemical properties and hole mobility measurements. The oxidation peaks at 1.2 V and 1.4 V were observed at the LS and ALS modified electrode, respectively. We studied the hole transport properties of LS and ALS using the space-charge-limited current method (SCLC). Average hole mobilities of 2.95 × 10−6 cm2 V−1 s−1 and 3.18 × 10−7 cm2 V−1 s−1 were estimated for LS and ALS, respectively. The above results indicated that LS and ALS are potential water soluble polymeric p-type semiconductors, and the hole transport property of LS is better than that of ALS. Based on the unique aggregation behavior and hole mobility property described above which will facilitate charge transport, water soluble PEDOT:LS and PEDOT:ALS were prepared and applied as the hole extraction layer (HEL) in polymer solar cells. The PCE decreased with a decrease of the phenolic hydroxyl group content (–OH), which suggested that –OH is important for the strength of the PCE. The application properties were consistent with the results of the aggregation behavior and electron transfer properties. The power conversion efficiency (PCE) of 5.19% from PEDOT:LS-1:
1 as the HTL was achieved with a device structure of ITO/HEL/PTB7:PC71BM/Al in our study. Our results showed that the phenolic hydroxyl group content and conjugation structure of amorphous LS contribute to its promising potential as a dopant of semiconductors, such as PEDOT in organic electronics. Our results provide a novel perspective for the design of dopants for semiconductive polymers. In summary, the phenolic hydroxyl group of the polymer will provide hole transport capability due to its oxidation during device operation.
Based on our previous work,14,15 it is now well known that amorphous lignosulfonate (LS) exists as a small aggregate of nano-size in solution. However the unique block-like aggregate of LS in selective solvents is rarely reported and very different to nanospheres of LS. The high value-added application of LS is of great importance. We noticed an odd chemistry where lignin and lignosulfonate will be converted into an oxidized state with radicals, which can be detected by electron spin resonance (ESR).16–18 Inspired by the unique aggregation behaviour of LS and ALS via their self-assembly and the electron transfer process during the oxidation of LS, we proposed a study of the hole transport properties of LS and ALS. Based on the aggregation behaviour and electron transfer properties of LS and ALS, LS and ALS were used as dopants to disperse poly(3,4-ethylene dioxythiophene) (PEDOT) for preparing the conductive polymers PEDOT:LS and PEDOT:ALS.
During the past decades of development of organic electronic devices including polymeric light emitting diodes (PLEDs), organic solar cells (OSCs) and organic photovoltaics (OPVs), interface modifier materials played indispensable roles for both the anode and cathode.19–24 It is an exciting result that a power conversion efficiency (PCE) exceeding 10% has been demonstrated in a highly efficient single junction PSC with a poly[(9,9-bis(3,-(N,N-dimethylamino)propyl)-2,7-fluorene)-alt-2,7-(9,9–dioctylfluorene)] (PFN) modified cathode.25,26
In contrast, for the modification of the anode, poly(3,4-ethylene dioxythiophene):poly(styrene sulfonic acid) (PEDOT:PSS) acts as a hole transport material (HTM) and plays an indispensable role as one of the most widely employed HTMs to modify indium-tin oxide (ITO) anodes resulting in good performances.27 However, numerous alternative materials to PEDOT:PSS have been pursued because it is well known to corrode ITO at elevated temperatures due to its high acidity.28 New solution-processable HTMs are still in demand and chemists have made great efforts to explore new alternative materials.29–36 Recently, we reported that PEDOT:SL as a hole transporting material exhibited promising performance in polymer solar cells.37 In order to study the effect of –OH and the aggregation behaviour of lignosulfonate for the performance of PSCs, we chose LS and ALSs as starting materials in our previous manuscript14 to study the effect in detail. The motivation for this is also based on the following considerations.
Firstly, lignin,38–40 the second most abundant plant resource, has three types of phenol derivatives including p-coumaryl alcohol, coniferyl alcohol, and sinapyl alcohol, which can be oxidized into radicals or radical cations. The electron transfer process accompanied with oxidation provides a potential for lignin to act as the hole transport material. The traditional and classical hole transport/injection layer (HTL/HIL) poly-N-vinylcarbazole (PVK) contains an electron-rich building block carbazole based derivative. However, there are rarely reports of hole injection/transport layers based on electron-rich compounds such as phenol and its derivatives. It is well known that most HTMs will form radical cations during oxidation as shown in Scheme 1. PVK is one of the most widely studied HTMs in previous works. It is noteworthy finding that the highest occupied molecular orbital (HOMO) of PVK is −5.6 eV. We propose LS can act as the HTM/HIT like PVK. The HOMO energy level of LS is also −5.6 eV and it is a potentially good candidate for an anode modifier. Secondly, the high acidity of PEDOT:PSS is caused by the anionic dispersant PSS, however, the limited sulfonation degree of LS and ALS will provide a high pH for the dispersed conductive polymer, which will reduce its corrosion of ITO. Thirdly, as a water soluble polymer from biomass, lignosulfonate showed good dispersion properties in various industrial fields such as dimethomorph water-dispersible granule,41 cement–water systems,42 TiO2 suspension43 and coal water slurry as shown by our group.14
In the following report, we find that LS and ALS could form a unique block-like self-assembly in selective solvents. The aggregation behavior and formation mechanism were investigated in detail. The block-like aggregates from ALS were obviously larger than those from LS. It suggested that alkyl chain cross-linked polymerization of LS may lead to the intensive aggregation behavior of ALS. Furthermore, water soluble PEDOT:LS and PEDOT:ALS were prepared and applied as hole extraction layers in polymer solar cells (PSCs). The results indicated that the content of phenolic hydroxyl group (–OH) affects the power conversion efficiency (PCE) of PSCs, and a PCE of 5.19% from PEDOT:LS-1:
1 was achieved with the device structure ITO/HEL/PTB7:PC71BM/Al. Our results showed that LS might be promising as a potential dopant of semiconductors, such as PEDOT in organic electronics. The underlying mechanism was also studied and discussed in detail.
The novelty of the block-like aggregate formation mechanism emerges by comparison to other lignin nano- and micro-structures, which was investigated by SEM as shown in Fig. 1. It is well known that lignosulfonate exists as nano-sized oval-shaped aggregates in a dilute water solution.14,15 As shown in Fig. 1a and d, a lot of nano-aggregates were observed by SEM in the first stage. The diameter was approximately 20 nm. When ethanol was added into the aqueous solution, the degree of aggregation from LS and ALS was obviously different from each other. Structures consisted of many nano-aggregates yielding a block-like self-assembly as shown in the second stage (Fig. 1b and e). Finally, the homogeneous and unique block-like self-assembly was formed both from LS and ALS as shown in Fig. 1c and f. However, block-like self-assemblies of nano-size were observed from LS, and that of micro-size were observed from ALS. Similar SEM images are also shown in Fig. S1.† It is suggested that alkyl chain cross-linked polymerization of LS may lead to the intensive aggregation behavior of ALS. Lignosulfonate, as an amorphous polymer, is an amphiphilic polymer with many aromatic benzene rings, which are easy to aggregate in selective solvents via CH–π and π–π interactions to yield the unique self-assembly.44
In order to investigate the formation mechanism of block-like self-assembly in more detail, TEM and DLS were conducted in this study. It was confirmed that LS could self-assemble into nano-sized block-like aggregates in a H2O/ethanol solution and ALS could form a micro-sized block-like self-assembly as shown in Fig. 2. The block-like structure containing many compacted nano-aggregates from LS and ALS seemed to be homogeneous and well-defined. A dynamic light scattering study of block-like aggregates can give important information about the solution self-assembly process. As shown in Fig. S2,† the average diameter of the block-like aggregates from the LS solution was about 300 nm and that from the ALS solution was 9 μm, which was consistent with the electron microscopy results above. These results indicated that the block-like structure was formed via self-assembly in selective mixed solvents of water and ethanol and the aggregation degree of ALS is obviously different compared with LS.
![]() | ||
Fig. 2 Typical TEM images of the homogeneous nano-sized block-like self-assembly from LS (a) and the micro-sized block-like self-assembly from ALS (b). |
X-ray photoelectron spectroscopy (XPS) measurements were conducted to test the element distribution of the block-like aggregates. As shown in Fig. 3a, high proportions of carbon and oxygen elements were detected from the block-like structures, which further supported the above result that the block-like self-assembly was formed from LS and ALS.
To determine the regular intrinsic characteristics of the block-like structure, small-angle X-ray scattering (SAXS) measurements were conducted by dropping a sample solution of the block-like self-assembly on a silicon wafer and drying at room temperature. As shown in Fig. 3b, at low angles, strong reflections (8.1° and 16.2°) were detected by SAXS. All the above results indicated that the block-like structure had significant reflections. It is also further supported that the block-like self-assembly was fabricated from LS and ALS.
Cyclic voltammetry (CV) was used to study the oxidative activity of LS and ALS. The cyclic voltammograms of the LS and ALS film in a 0.1 M Bu4NPF6 (in dichloromethane) solution were used to investigate the electrochemical behaviour of LS and ALS as shown in Fig. 4. The oxidation peaks at 1.2 V and 1.4 V were observed at the LS and ALS modified electrode, respectively. It suggested that the oxidative activity of LS is better than that of ALS. The reaction mechanism for the reaction of LS and ALS at the surface of the electrode was proposed. LS was proposed to be oxidized to form radical cations. Meanwhile, the phenolic hydroxyl group (–OH) of LS might be also oxidized into phenol radicals. The –OH content of LS is greater than that of ALS, which could lead to the better oxidative activity of LS. The electron transfer process provides a new concept for the design of HTM molecules.
In order to make a quantitative evaluation of the hole transport properties of LS and ALS materials, the hole mobility was measured by testing J–V characteristics of the hole-only devices with the device structure ITO/MoO3/sample/MoO3/Al as shown in the structure diagram inserted in Fig. 5. As a wide band gap semiconductor, MoO3 is used to assist the hole transport to the ITO anode and block the electrons injected from the Al cathode at the same time. The observed dark current–voltage curve was then fitted by using the space-charge-limited current (SCLC) model, which is described by the equation as follows:
J = (9/8)εrε0μ(V2/d3) |
![]() | ||
Fig. 5 The J–V curves of hole-only devices with a SCLC fitting from LS and ALS (the structure of hole-only devices is inserted as a picture in the top-left corner). |
In the equation above, ε0 is the dielectric permittivity of free space, εr is the relative permittivity of the sample, μ is the mobility, and d is the thickness of the sample. The hole mobility value was obtained by the SCLC equation with the detailed data listed in Fig. 5 and Table 1.
Samples | Thickness (L) (nm) | Slope (ρ) | Hole-mobility (cm2 V−1 s−1) |
---|---|---|---|
LS | 35 | 13.86 | 2.95 × 10−6 |
ALS | 50 | 2.45 | 3.18 × 10−7 |
As can be seen from Fig. 5 and Table 1,the hole mobility 2.95 × 10−6 cm2 V−1 s−1, estimated for LS, is nearly one order of magnitude higher than that of ALS (3.18 × 10−7 cm2 V−1 s−1). The result indicates that the LS and ALS are potential water soluble organic semiconductors with hole transporting properties. Moreover, LS with a greater content of phenolic groups, has a higher hole mobility than ALS with a smaller content of phenolic groups. This suggested that the phenolic group contributes to the hole transporting property, which is in good agreement with the electrochemical property results described above.
UV-vis absorption spectra of PEDOT:LS and PEDOT:ALS aqueous dispersions are shown in Fig. S3.† Because of the higher phenolic hydroxyl group content of LS, the absorption intensity of PEDOT:LS from 250 to 300 nm is obviously stronger than that of PEDOT:ALS. The UV spectra of PEDOT:LS and PEDOT:ALS aqueous dispersions showed the presence of a bipolaron absorption band at 800 nm, which was ascribed to the π–π transition in the PEDOT polymer chain.45 The broad absorption from 600 to 900 nm was also detected in both PEDOT:LS and PEDOT:ALS aqueous dispersions. It further confirmed that PEDOT:LS and PEDOT:ALS were successfully prepared in our study.
The cyclic voltammograms of the PEDOT:LS film and PEDOT:ALS film in a 0.1 M Bu4NPF6 (in dichloromethane) solution were also obtained as shown in Fig. 6. Compared with that of PEDOT:ALS, an obvious oxidation peak at 0.65 V was observed at the PEDOT:LS modified electrode. Two oxidation potentials at 0.65 V and 0.75 V were observed at the PEDOT:LS and PEDOT:ALS modified electrode, respectively. The HOMO value of PEDOT:LS and PEDOT:ALS were calculated as −5.05 eV and −5.15 eV, respectively. It indicated that LS has a positive effect on the conductive polymer PEDOT and LS with a higher –OH content facilitates the hole transfer of PEDOT:LS. The corresponding oxidation mechanism was proposed as shown in Fig. 7. It encouraged us to study its potential application in organic electronics.
![]() | ||
Fig. 6 Cyclic voltammograms of the PEDOT:LS film and PEDOT:ALS film in a 0.1 M Bu4NPF6 DCM solution. |
To evaluate the hole transport performance of PEDOT:LS and PEDOT:ALS, PSCs with PEDOT:LS and PEDOT:ALS as the anode modifier were fabricated. The detailed device architecture of the PSCs and current density (J)–voltage (V) curves of the PSCs with different HTMs are shown in Fig. 8. The power conversion efficiency (PCE), short-circuit current density (JSC), open-circuit voltage (VOC) and fill factor (FF) of the PSCs are given in Table 2. PEDOT only showed a poor PCE of 2.91% with a FF of 48.04%. The same devices (ITO/HEL/PTB7:PC71BM/Al) with the PEDOT:PSS modified anode showed a JSC of 12.77, VOC of 0.72 and PCE of 4.28% with a FF of 46.40% as shown in ref. 46. The PCE of the PSCs in a conventional device structure ITO/PEDOT:PSS/PTB7:PC71BM/Al was 4.50%, as reported previously,47 and are shown in Table 2. The PCEs of the device with PEDOT:LS and PEDOT:ALSs with different mass ratios in the device structure ITO/PEDOT:PSS/PTB7:PC71BM/Al were all investigated in this study as shown in Table 2. In our previous manuscript,14 the content of –OH decreased gradually from LS to ALS3. As can be seen from Table 2, the PCEs of the device with PEDOT:LS-1:
1, PEDOT:ALS1-1
:
1, PEDOT:ALS2-1
:
1 and PEDOT:ALS3-1
:
1 were 5.19%, 4.75%, 3.49% and 3.11%, respectively. The PCEs decreased with a decrease of –OH content, which indicated that –OH is important for the electron transfer process. The results were consistent with the results of CV and hole mobility. In addition, when the mass ratio of PEDOT:LS and PEDOT:ALS1 was 1
:
2, the PCEs of the device with PEDOT:LS-1
:
2 and PEDOT:ALS-1
:
2 were 5.02% and 3.73% which were lower than that of the device using PEDOT:LS-1
:
1 and PEDOT:ALS-1
:
1. It is noteworthy that when PEDOT:LS-1
:
1 was applied, a PCE of 5.19% with a JSC of 15.06 mA cm−1, VOC of 0.58 V and FF of 58.87% was obtained. The PCE of PEDOT:LS-1
:
1 (5.19%) was higher than that of PEDOT:PSS46 (4.50%). The results indicate that LS might be promising as a potential dopant in semiconductors. It encourages us to study its potential further in the future. We proposed the possible mechanism based the following three aspects.
![]() | ||
Fig. 8 (a) Device architecture of polymer solar cell (PSC). (b) J–V curves of PSCs with PEDOT only, PEDOT:LS and PEDOT:ALSs with different mass ratios of ITO/HTM/PTB7:PC71BM/Al in the devices. |
Anode | VOC (V) | JSC (mA cm−2) | FF (%) | PCE (%) |
---|---|---|---|---|
PEDOT:PSS46 | 0.72 | 12.77 | 46.40 | 4.28 |
PEDOT:PSS47 | 0.62 | 14.58 | 50.00 | 4.50 |
None | 0.43 | 14.12 | 48.04 | 2.91 |
PEDOT:LS-1![]() ![]() |
0.58 | 15.06 | 58.87 | 5.19 |
PEDOT:LS-1![]() ![]() |
0.65 | 13.43 | 57.55 | 5.02 |
PEDOT:ALS1-1![]() ![]() |
0.57 | 14.69 | 56.40 | 4.75 |
PEDOT:ALS1-1![]() ![]() |
0.56 | 12.20 | 54.55 | 3.73 |
PEDOT:ALS2-1![]() ![]() |
0.68 | 11.17 | 45.88 | 3.49 |
PEDOT:ALS3-1![]() ![]() |
0.68 | 10.96 | 41.74 | 3.11 |
On one hand, from the electrochemical properties and hole mobilities of LS and ALS, both LS and ALS have potential as semiconductors for hole collection in PSCs. However, the hole mobility of ALS was much lower than that of LS which suggested that the phenolic group content could affect the hole transporting property. Combined with the unique aggregation behaviour, the aggregation degree of ALS is obviously different compared with LS. PEDOT:LS and PEDOT:ALS were applied as novel and potential hole extraction layers (HELs) in polymer solar cells.
On the other hand, in our work, an alkyl chain was introduced in the phenolic group of LS to obtain ALSs; the results above indicated that the phenolic group content could affect the hole transporting property and electron transfer property as shown in Fig. 4 and 5. The oxidation process of PEDOT:LS and PEDOT:ALS was also investigated in our study as shown in Fig. 6. As can be seen in Fig. 9, the HOMO energy level values were 5.0 eV, 5.05 eV and 5.15 eV for PEDOT:PSS, PEDOT:LS and PEDOT:ALS, respectively, which suggested that there are smaller energy gaps in thin films for PEDOT:LS compared to PEDOT:ALS. This is very important for hole transport. Therefore, PEDOT:LS exhibited a better power conversion efficiency than PEDOT:ALS acting as the HEL in polymer solar cells.
![]() | ||
Fig. 9 HOMO energy levels of ITO, PEDOT, PEDOT:LS, PEDOT:ALS and PTB7 (HOMO of PEDOT:LS and PEDOT:ALS were calculated as −5.05 eV and −5.15 eV, respectively, as shown in Fig. 6). |
Finally, as studied previously, ALS is easier than LS to aggregate, especially in order to fabricate unique block-like aggregates with micro-sizes in selective solvents. The aggregation behavior also affects the hole transporting property of conductive PEDOT. Therefore, we studied the surface morphologies of the PEDOT:LS film and PEDOT:ALS by AFM as shown in Fig. 10a–f. There is a significant difference between them. Overall, the AFM images of PEDOT:ALS films were rough, which was ascribed to the intensive aggregation capability of ALS. The AFM images of PEDOT:LS films were more homogeneous and compacted than that of PEDOT:ALS films. The particle size of PEDOT:LS was also relatively smaller than that of PEDOT:ALS. In the above results, the more homogeneous, smaller sized and compact nano-aggregates might facilitate charge transport of PEDOT:LS polymers in a film. It is an interesting result that LS can act as a dopant of PEDOT even though it has such a complex, disordered and amorphous structure. Compared to PSS, which has a regular structure, the stronger crystallization character and oxidation behaviors of LS might have contributed to the unexpected hole transport of the PEDOT:LS film. Moreover, the pH value of the PEDOT:ALS aqueous dispersion (pH 3.9) was higher than that of PEDOT:PSS (pH 1.9), which is conducive to reduce the corrosion of ITO during device operation.
In summary, based on the unique aggregation behavior, electron transfer property and hole mobility of LS compared with ALS, LS showed a novel application potential as a dopant for water soluble polymeric semiconductors. PEDOT:LS showed a promising performance as a hole-transport material in polymer solar cells (PSCs), which is comparable with that of conventional PEDOT:PSS. The results have rarely been reported, to date. LS, as a novel hole transport material from a renewable bioresource, might be a potential water soluble polymeric semiconductor. The dopant design concept of PEDOT provides a promising strategy to develop stable water soluble PEDOT semiconductive polymers, which will accelerate the commercialization of solution processable organic electronics in the future.
Atomic force microscopy (AFM) images were observed using a Park XE-100 instrument in tapping mode. The AFM samples were prepared by dropping the sample solution on the substrate as slow as possible and drying under room temperature for 24 hours.
Transmission electron microscopy (TEM) images were obtained using a HITACHI H-7650 electron microscope with an accelerating voltage of 200 kV. The TEM samples were prepared by dropping diluted sample solution onto copper grids coated with a thin carbon film.
Dynamic light scattering (DLS) experiments were performed on a Zeta PALS instrument (Brookhaver, America). The concentration of the samples was 0.05 mg mL−1 in H2O/ethanol (v/v, 1:
3) at around pH 7.0.
The block-like self-assemblies for X-ray photoelectron spectroscopy (XPS) were prepared by dropping the sample solutions on tinfoil and drying naturally at room temperature.
The block-like self-assemblies for small-angle X-ray scattering (SAXS) were prepared by dropping the sample solutions on a Si substrate and drying naturally at room temperature.
Cyclic voltammetry measurement was conducted as follows: a glassy carbon electrode was first polished carefully with alumina powder to a mirror finished surface and rinsed with distilled water repetitively. LS and ALS solutions were prepared by dissolving a 10 mg sample in 1 mL distilled water. Then the sample film was deposited at the surface of the clean glassy carbon electrode. PEDOT:LS and PEDOT:ALS films were directly deposited at the surface of the clean glassy carbon electrode. The resulting electrode was immersed in 0.1 M Bu4NPF6 DCM solutions, and was stabilized in 0.1 M Bu4NPF6 DCM solutions by scanning the potential between −0.6 and +2.0 V at a scan rate of 100 mV s−1.
The hole mobilities of LS and ALS were measured using the space-charge-limited current (SCLC) method by testing J–V characteristics of the hole-only device structure: ITO/MoO3 (10 nm)/sample/MoO3 (10 nm)/Al (100 nm). The film of the sample was spin-coated with a concentration of 80 mg mL−1 and the solvent of the sample is deionized water.
For the fabrication and characterization of OPVs:ITO-coated glass substrates, they were first cleaned by sonication in acetone, detergent, deionized water, and isopropyl alcohol and dried in a nitrogen stream, followed by an oxygen plasma treatment. In order to fabricate photovoltaic devices, a thin hole-transportation layer (ca. 40 nm) of PEDOT:SL or PEDOT:ALS (filtered at 0.45 μm) was spin-cast on the pre-cleaned ITO-coated glass substrates and baked at 120 °C for 20 min under ambient conditions. The active layer PTB7:PC71BM (10:
15 mg mL−1) was prepared by spin-casting a chlorobenzene solution with the addition of a small amount of DIO (CB
:
DIO = 100
:
3, V/V) at 1500 rpm for 30 s in a dry box. The thickness of the PTB7:PC71BM layer was about 100 nm. 4 h later, methanol was spin-coated on the active layer at 2000 rpm for 30 s. The Al electrodes were thermally deposited for 100 nm through a mask in a vacuum (<5 × 10−4 Pa). All steps except for the processing of HTMs were performed in a glove box. The effective device area was about 0.16 cm2. The current density–voltage (J–V) characteristics were measured using a Keithley 2400 source meter. The photovoltaic devices were characterized using a calibrated AM1.5 G solar simulator (Oriel model 91192), under a light intensity of 100 mW cm−2.
Footnote |
† Electronic supplementary information (ESI) available: The results including SEM images of various block-like self-assemblies from LS and ALS; DLS measurement of the LS solution and ALS solution in H2O/EtOH (v/v, 1/3); proposed schematic for the polymerization of EDOT in the presence of LS and ALS; UV absorption spectra of PEDOT:LS and PEDOT:ALS aqueous dispersion. See DOI: 10.1039/c5ra19676k |
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