Mingguang Li‡
,
Wen Zhang‡,
Honglei Wang,
Lingfeng Chen,
Chao Zheng and
Runfeng Chen*
Key Laboratory for Organic Electronics and Information Displays, Institute of Advanced Materials, Jiangsu National Synergetic Innovation Center for Advanced Materials, Nanjing University of Posts and Telecommunications, Wenyuan Road, Nanjing, 210023, P. R. China. E-mail: iamrfchen@njupt.edu.cn
First published on 16th June 2017
The cathode interfacial layer (CIL) plays a vital role in enhancing the efficiency and lifetime performance of bulk heterojunction (BHJ) polymer solar cells (PSCs). Here, we compared the use of various organic semiconducting molecules, tris(8-hydroxyquinolinato) aluminum (Alq3), bathocuproine (BCP) and 1,3,5-tri(m-pyrid-3-yl-phenyl)benzene (TmPyPB), as CILs in PSCs and analyzed their influence on device performance. Compared to the inorganic LiF CIL-based PSCs, significantly higher photovoltaic performance was observed by using these organic CILs in both PTB7:PC71BM and P3HT:PC61BM PSCs. Specifically, TmPyPB CIL-based devices exhibit superior device stability and high power conversion efficiency (PCE) up to 7.96%. A systematic study on the effects of Frontier orbital energy levels, surface morphology, and electron mobility of CILs suggests that a relatively coarse interface morphology would be helpful in the formation of high-density interfacial defect states for efficient electron extraction and a high mobility is of central importance in facilitating electron collection for high PCEs. Moreover, a synergistic effect between the inorganic LiF and organic molecules in the dual-CIL could contribute to the further enhancement of PSC efficiency (8.01%) and ambient stability. This work reveals fundamental principles in regulating the functions of CILs and would hopefully promote the investigation and development of ideal organic CILs for high-performance PSCs.
Cathode interfacial layer (CIL), which is close to the metal cathode with low work function, influences significantly the electron extraction and transport processes, representing an effective way to improve the PSC performance. The contributions of CIL can be attributed to (1) suppressing the quenching of exciton at the metal electrode, (2) tuning the energy-level alignment at the interfaces for facile electron extraction, (3) protecting the active layer from damaging during the thermal deposition of metal cathode, (4) forming a passivating layer to resist oxygen and moisture diffusion. Many CIL materials including inorganic metal oxides (e.g., ZnO and TiOx),7–10 polymer/small-molecules,11–13 fullerene-based materials,14,15 and other alternatives16 have been reported and applied to optimize the device efficiency and stability. Among them, the electron transporting organic semiconductors that have been widely used in organic light emitting diodes (OLEDs),17–19 show particular advantages.20 These molecules with high electron mobility can be easily deposited by vacuum evaporation or solution-processing, generally demonstrating better PSC performance in comparison with the commonly used inorganic LiF CIL.21 However, in-depth understandings on the organic–metal interface and the internal correlations between CIL material properties, interface structure, contact state and type, and electron extraction and collection processes are still limited, which has hindered significantly the rational design and selection of ideal organic semiconducting CIL materials for the preparation of high-performance PSCs.
Here, we systematically investigated the relations between the organic CIL material properties and the PSC performance, focusing particularly on the effects of energy-level alignment, surface morphology, and electron mobility, based on a series of organic semiconducting molecules including tris(8-hydroxyquinolinato) aluminum (Alq3), 2,9-dimethyl-4,7-diphenyl-1,10-phenanthroline (BCP), and 1,3,5-tri(m-pyrid-3-yl-phenyl)benzene (TmPyPB) (Fig. 1a). Compared to LiF, these organic CIL molecules show improved device performance in both traditional blends of poly (3-hexylthiophene) (P3HT) and [6,6]-phenyl-C61-butyric acid methyl ester (PC61BM) and high-performance poly[[4,8-bis[(2-ethylhexyl)oxy] benzo [1,2-b:4,5-b′]dithiophene-2,6-diyl][3-fluoro-2-[(2-ethylhexyl) carbonyl] thieno[3,4-b]thiophenediyl]] (PTB7) and [6,6]-phenyl-C71-butyric acid methyl ester (PC71BM) systems. TmPyPB-based PSCs has the highest device stability and PCE values up to 7.96%, due to its high electron mobility and the relatively coarse surface morphology for high-density organic/metal interface defect states in facilitating the electron transport and extraction, respectively. The combination of inorganic LiF CIL and organic TmPyPB CIL further enhances hole-blocking ability to suppress charge carrier recombination and protects the underlying PSC active layer from damaging under the ambient environment, leading to improved PCE of 8.01% and device stability in dual-CIL architecture.
Based on the typical BHJ PSC structure of ITO/PEDOT:PSS/PTB7:PC71BM/CIL/Al (inset of Fig. 2) with an active area of 9 mm2 (Fig. S1†), the influence of the organic CILs on the photovoltaic properties were studied. These devices exhibit similar open-circuit voltages (Voc) of 0.75 ± 0.02 V, but varied short-circuit currents (Jsc) from 14.18 to 16.62 mA cm−2 and PCE from 6.84% to 8.01% after the incorporation of different CILs. Compared to the LiF-only CIL reference device, the use of organic CILs results in comparable Voc and fill factor (FF) but significantly increased Jsc, and thus improved PCE in the order of LiF < BCP < Alq3 < TmPyPB < TmPyPB/LiF; this selectively enhanced Jsc can also be found in the literature using other organic CIL molecules (Fig. 2a).20,22,23 As shown in Table 1, series resistance (Rs) decreases from 7.5 Ω cm2 for LiF-only device to 5.3 Ω cm2 for TmPyPB/LiF dual-CIL device, indicating a reduced semiconductor bulk resistance and a better metal/semiconductor interface connection, which should be responsible for the enhanced Jsc.24 As to the slightly varied Voc, different natures of these CIL materials may influence the charge recombination dynamics of the photovoltaic materials in the active layer, leading to disturbed Voc in a small range of variation.25
System | CILs | Voc [V] | Jsc [mA cm−2] | FF [%] | PCE [%] | Rs [Ω cm2] | Rsh [Ω cm2] |
---|---|---|---|---|---|---|---|
PTB7:PC71BM | LiF | 0.74 | 14.22 | 62.8 | 6.68 | 7.5 | 506.9 |
BCP | 0.77 | 14.18 | 62.6 | 6.84 | 7.9 | 664.7 | |
Alq3 | 0.76 | 14.27 | 66.9 | 7.26 | 6.1 | 879.4 | |
TmPyPB | 0.77 | 15.89 | 64.9 | 7.96 | 6.6 | 808.5 | |
TmPyPB/LiF | 0.73 | 16.62 | 66.0 | 8.01 | 5.3 | 857.9 | |
P3HT:PC61BM | LiF | 0.64 | 8.41 | 59.7 | 3.27 | 11.5 | 547.1 |
BCP | 0.65 | 8.86 | 57.0 | 3.32 | 11.1 | 480.6 | |
Alq3 | 0.63 | 9.34 | 60.1 | 3.53 | 11.0 | 460.4 | |
TmPyPB | 0.63 | 9.74 | 58.0 | 3.60 | 11.2 | 472.2 | |
TmPyPB/LiF | 0.63 | 9.80 | 62.2 | 3.80 | 10.5 | 531.5 |
With the deepest HOMO of TmPyPB CIL to block effectively the hole diffusion towards the cathode side, the highest Jsc and PCE values were resulted, and these values can be further improved to 16.62 mA cm−2 and 8.01% when using the TmPyPB/LiF dual-CIL. The low PSC performance of Alq3 CIL should be related to its unmatched HOMO, which is too low (lower than that of PC61BM in the active layer) to prevent the charge recombination in CIL. The external quantum efficiency (EQE) spectra of the five PSC devices with different CILs were measured (Fig. 2b). It was found that the EQE spectrum with similar sharp enhances in the whole wavelength range in a same order to the Jsc enhancement of BCP < Alq3 < TmPyPB < TmPyPB/LiF. Specifically, LiF-only device exhibits a maximum of ∼59% at 560 nm, while that of TmPyPB/LiF dual-CIL device reaches a maximum of ∼63% at 540 nm with much more significant improvement at the wavelength band of 350–680 nm. To reveal the origin of the increased Jsc, EQE and PCEs using various organic CILs, the UV-vis absorption of PTB7:PC71BM blend films with CILs were characterized (Fig. S2†). Negligible absorption difference of these films was observed, suggesting there are limited effects of CILs on the light harvesting for increased Jsc and PCE.
As to the influence of CILs on the PSC stability (Fig. 2c), the LiF-only device suffered from rapid degradation in PCE value within 72 h. In contrast, TmPyPB-only device and TmPyPB/LiF dual-CIL device exhibit significant lifetime improvement, maintaining up to 90% of its original value after 72 h in air without any encapsulation. Thus, air-stability modification is identified to be correlated with the introduced organic CIL, which could effectively block the oxygen and water from permeating through the CIL. The positive effect of Alq3 and TmPyPB on the device stability has also been reported in other PSC systems.22,26 However, it should be noted that the introduction of BCP layer cannot contribute much to the improvement of device stability, probably because BCP thin film can readily crystallize especially in the presence of moisture,22,27 leading to the rapid degradation of device performance.
To further elucidate the factors responsible for the enhanced Jsc value, the AFM height images of different CILs over PTB7:PC71BM blend films were investigated (Fig. 3), because it is well-known that interface morphology may influence the organic–metal contact, charge transport, and optical property significantly.28,29 After deposition of a thin layer of LiF (1 nm), the CIL exhibits very uniform surface morphology with rms roughness of 3.29 nm (Fig. 3a), which is very close to that of the original surface of PTB7:PC71BM active layer (Fig. S3†). The vacuum deposition of organic semiconductor CILs of BCP (5 nm) and Alq3 (5 nm) (Fig. 3b and c) also show the uniform surface morphology with only slightly increased film roughness (rms) of 4.04 and 3.63 nm, respectively. In contrast, the film morphology changes significantly when TmPyPB was deposited as a CIL (8 nm) on the active layer (Fig. 3d). As magnified in Fig. S4,† “island” structure with the diameter about 100 nm was observed and the rms roughness reached 6.68 nm. When another LiF CIL (1 nm) was deposited onto the TmPyPB CIL to form the dual-CIL (Fig. 3e and f), the “island” structure remains with similar size but decreased film roughness (rms = 5.72 nm).
Fig. 3 AFM height images (10.0 μm × 10.0 μm) of (a) LiF, (b) BCP, (c) Alq3, (d) TmPyPB and (e) TmPyPB/LiF dual CILs on PTB7:PC71BM based PSCs. (f) The magnified AFM images (2.0 μm × 2.0 μm) of (e). |
As previously reported, the photogenerated electrons can only be transported from the LUMO of acceptor molecules into the metal cathode through the defect states below the LUMO of CIL materials when the LUMO of acceptor molecules lies below that of CIL materials by ∼1.0 eV.30 The so-called “defect states” in the CILs are induced by the thermalization of the hot Al atoms during deposition of the electrode.31 In this sense, the rough surface morphology with high density of “island” structures, which can maximize the contact area between CIL and Al cathode, are expected to be advantageous for the creation of higher density of defect states responsible for the electron extraction.32 This should be an important reason for the highest PSC performance observed when using the TmPyPB-based CIL.
Although the Frontier orbital energy level analysis of the PSC layers gives a good prediction of the highest PSC performance by using TmPyPB-based CIL, it cannot explain the poor performance using BCP CIL (PCE = 6.84%), because BCP has very close HOMO (−6.5 eV) and LUMO (−3.0 eV) to those of TmPyPB (−6.7 eV and −2.7 eV) and its interface morphology is also similar to that of Alq3. Considering central role of CIL in transporting electron and blocking hole from the active layer to the metal cathode, the charge mobility of the CIL materials must be crucial in influencing CIL performance. From the literature reports (Table S1†), the highest electron mobility can be found in TmPyPB (1.0 × 10−3 cm2 V−1 S−1),22 which is coincident with our measurements based on electron-only devices using the space charge limited current (SCLC) model (Fig. S5†). Therefore, a relatively low electron mobility (5.0 × 10−6 cm2 V−1 S−1) of BCP33 should be a main reason for its lowest PCE, although BCP has acceptable Frontier orbital energy levels and uniform surface morphology. The high electron mobility of TmPyPB guarantees the efficient electron transport during the charge collection process for the high PCEs.
The J–V characteristics of PTB7:PC71BM PSCs were further measured in the dark condition (Fig. 4a) to investigate the effective injection current that may be responsible for the prominently enhanced PCEs of TmPyPB-based devices. The high rectification factor (23288 at ±1.5 V) and low leakage current (6.62 × 10−3 mA cm−2 at −1.5 V) of the TmPyPB-only device clearly implies its excellent diode property (i.e. transporting electrons and blocking the holes, as shown in Fig. 4b). Similar J–V property under dark condition was observed for TmPyPB/LiF dual-CIL device with rectification factor up to 26008 at ±1.5 V. Compared to LiF-only device with rectification factor around 355 at ±1.5 V, the introduction of Alq3 CIL also results in enhanced diode property to some extent, but the BCP CIL shows almost no diode character enhancement. Since the shunt resistance (Rsh) of PSC devices usually reflects the degree of leakage current, these results observed in dark condition can be also supported by the variation of Rsh shown in Table 1. The introduction of organic CILs results in exceptionally enlarged Rsh from 506.9 Ω cm2 for LiF to more than 800 Ω cm2 (879.4 Ω cm2 for Alq3, 808.5 Ω cm2 for TmPyPB and 857.9 Ω cm2 for TmPyPB/LiF), demonstrating clearly the positive effect of organic CILs in restraining the leakage current under reverse bias.24 These observations, which are in line with the electron mobility study, suggest again the profound impacts of electron mobility on the performance of CILs for PSCs.
Fig. 4 (a) J–V characteristics of PSCs with different CILs measured under dark conditions. (b) The schematic representation of the role of CIL on charge collection. |
The enhancement effects of organic CILs on PSC performance were also observed in classical P3HT:PC61BM system. Similar rules in influencing device performance and air-stability are still valid in this different PSC system (Fig. S6†). From the summarized photovoltaic parameters in Table 1, TmPyPB/LiF dual-CIL, which has the best device performance, can benefit from both sides of organic and inorganic parts as well as their synergistic effects, offering a high-performance organic/inorganic CIL configuration to improve charge carrier extraction and transportation for varied PSCs with improved PCEs.
The successful attempt in using organic CILs and organic/inorganic dual-CILs to enhance the PSC performance (Fig. 4b) makes it possible to shed light on selecting or designing suitable organic CIL materials. An ideal CIL material should have (1) sufficient defect states to facilitate the electron extraction from the acceptor material, (2) high electron mobility to transport the extracted electron to the surface of metal cathode, (3) deep HOMO and low hole mobility to block the hole injection to the CIL and transport to the cathode. To this end, a relatively rough CIL morphology is expected to produce more defect states, while the LUMO energy level has limited effects on the electron extraction; high intrinsic electron mobility of the CIL material is important for facile electron transport to the cathode; deep HOMO of the CIL material is required to block the hole injection from the active layer and to prevent the recombination in the CIL; the CIL layer should be stable and compact to protect the active layer by resisting oxygen and moisture diffusion for high device stability.
Footnotes |
† Electronic supplementary information (ESI) available: UV-vis absorption spectra of PTB7:PC71BM blend films; fabrication and measurement of electron-only devices; The J–V curves and ambient stability characteristics of P3HT:PC61BM based PSCs. See DOI: 10.1039/c7ra04586g |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2017 |