|Hybrid polymer/ZnO solar cells sensitized by PbS quantum dots.|
|Jump to Full Text|
|PMID: 22313746 Owner: NLM Status: PubMed-not-MEDLINE|
|Poly[2-methoxy-5-(2-ethylhexyloxy-p-phenylenevinylene)]/ZnO nanorod hybrid solar cells consisting of PbS quantum dots [QDs] prepared by a chemical bath deposition method were fabricated. An optimum coating of the QDs on the ZnO nanorods could strongly improve the performance of the solar cells. A maximum power conversion efficiency of 0.42% was achieved for the PbS QDs' sensitive solar cell coated by 4 cycles, which was increased almost five times compared with the solar cell without using PbS QDs. The improved efficiency is attributed to the cascade structure formed by the PbS QD coating, which results in enhanced open-circuit voltage and exciton dissociation efficiency.|
|Lidan Wang; Dongxu Zhao; Zisheng Su; Dezhen Shen|
Related Documents :
|22553656 - Mechanisms of inhibition of elemene on human lens epithelial cell proliferation in vitro.
19836146 - The human superorganism - of microbes and men.
12646146 - Gastrulation: partaking of the bottle.
19726756 - An alpaca single-domain antibody blocks filopodia formation by obstructing l-plastin-me...
9744536 - Effects of cr(vi) on the expression of the oxidative stress genes in human lung cells.
18647166 - Tsr-gfp accumulates linearly with time at cell poles, and can be used to differentiate ...
|Type: Journal Article Date: 2012-02-07|
|Title: Nanoscale research letters Volume: 7 ISSN: 1556-276X ISO Abbreviation: Nanoscale Res Lett Publication Date: 2012|
|Created Date: 2012-03-02 Completed Date: 2012-10-02 Revised Date: 2012-11-09|
Medline Journal Info:
|Nlm Unique ID: 101279750 Medline TA: Nanoscale Res Lett Country: United States|
|Languages: eng Pagination: 106 Citation Subset: -|
|State Key Laboratory of Luminescence and Applications, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, People's Republic of China. email@example.com.|
|APA/MLA Format Download EndNote Download BibTex|
Journal ID (nlm-ta): Nanoscale Res Lett
Copyright ©2012 Wang et al; licensee Springer.
Received Day: 16 Month: 9 Year: 2011
Accepted Day: 7 Month: 2 Year: 2012
collection publication date: Year: 2012
Electronic publication date: Day: 7 Month: 2 Year: 2012
Volume: 7 Issue: 1
First Page: 106 Last Page: 106
Publisher Id: 1556-276X-7-106
PubMed Id: 22313746
|Hybrid polymer/ZnO solar cells sensitized by PbS quantum dots|
|Lidan Wang12||Email: firstname.lastname@example.org|
|Dongxu Zhao1||Email: email@example.com|
|Zisheng Su1||Email: firstname.lastname@example.org|
|Dezhen Shen1||Email: email@example.com|
1State Key Laboratory of Luminescence and Applications, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, People's Republic of China
2Graduate School of Chinese Academy of Sciences, Beijing 100039, People's Republic of China
Hybrid polymer solar cell is a promising photovoltaic technology, offering environmental stability, low-cost manufacturing, and versatile applicability [1-3]. The solution processing of polymer organic photovoltaic devices may offer an inexpensive technology to fabricate solar cells with large areas. Hybrid polymer-inorganic solar cells utilize the high electron mobility inorganic phase to overcome charge-transport limitations associated with organic materials. Zinc oxide [ZnO] has been regarded as an excellent semiconductor material for the solar cell due to its high electron mobility as well as the high chemical and thermal stability [4,5]. Compared with ZnO bulk materials, one-dimensional nanostructures have some special advantages for optoelectronic devices including the large surface area to significantly increase the junction area, the enhanced polarization dependence, and the improved carrier confinement in one dimension. Various polymer/ZnO hybrid solar cells have been reported [1,6]. However, the power conversion efficiencies [ηP] of these devices are still low and need to be further enhanced [4,7].
Pursuing high efficiency is indeed a core task for hybrid solar cell systems, and one of the current key issues is to search the suitable panchromatic sensitizers for enhancing the light harvest under a visible light region. In addition to traditional dye sensitizers, semiconductor quantum dots [QDs] have been researched as possible alternative sensitizers due to their high expectation of having the following advantages over molecular dyes: (1) facile tuning of effective bandgaps down to the infrared [IR] range by changing their sizes and compositions, (2) higher stability and resistivity toward oxygen and water over molecular counterparts, (3) new possibilities for making multilayer or hybrid sensitizers, and (4) new phenomena such as multiple exciton generation and use of energy transfer-based charge collection as well as direct charge transfer schemes. By now, many experiments have proved that it is possible to utilize hot electrons to generate multiple electron-hole pairs per photon through the impact ionization effect by using QDs . The concept of QD sensitization has been considered to be of great promise in increasing the ηP of the organic/inorganic hybrid solar cells. Various semiconductor QDs such as CdS [8-10], CdSe [11,12], PbS [13,14], PbSe [15,16], and InP  have been adopted in the hybrid solar cells. The QD-sensitized ZnO nanorod-based liquid solar cells have been proposed, but few QD-sensitized organic/ZnO nanorod hybrid solar cells sensitized by PbS QDs have been reported in the literature. The possible reasons may be that the QDs synthesized by the conventional solution methods have some surfactant molecules on the surface, which may block the transfer of the photogenerated carriers in QDs, and the preparation of PbS QDs on the ZnO nanorods was extremely difficult due to the high acidity of the lead salt. In this paper, we designed a hybrid ZnO nanorod solar cell, in which a ZnO nanorod array with a diameter of 40 to 80 nm and a length of 200 to 300 nm served as the n-type semiconductor and poly[2-methoxy-5-(2-ethylhexyloxy-p-phenylenevinylene)] [MEH-PPV] was adopted as the hole transfer layer. A thin PbS QD layer was sandwiched between ZnO and MEH-PPV layers synthesized by the chemical bath deposition [CBD] method. When PbS was introduced as the QD sensitizer, a cascade energy alignment was formed in the hybrid solar cell, and a ηP as high as 0.42% was achieved.
Among the various techniques to grow one-dimensional ZnO nanostructures, the cost-effective electrodeposition  method was used in this work for the nanorod preparation with large areas because of the low-temperature processing, arbitrary substrate shapes, and precise control of the size of nanorods. Firstly, a seed layer of 30 nm was grown by RF magnetron sputtering on cleaned indium tin oxide [ITO]-coated glass substrates with a sheet resistance of 25 Ω/sq. Then, ZnO nanorods were electrodeposited in 0.005 M Zn(NO3)2 and 0.005 M hexamethylenetramine aqueous solutions. All depositions were carried out in a configured glass cell at 90°C, in which the ITO substrate, a platinum plate, and an Ag/AgCl electrode in a saturated KCl solution served as the working electrode, the counter electrode, and the reference electrode, respectively. All electrodepositions were done at a potential of -0.9 V vs. the reference electrode. The durations of the deposition were 20 min. The PbS quantum dots were deposited by the simple CBD method. The CBD process involved dipping the prepared ZnO nanorod array substrate in a methanol solution consisting of 0.01 M lead acetate for 5 min and dipping it in another methanol solution consisting of 0.005 M Na2S for 10 min. After each step, the substrate was rinsed with methanol. The two-step dipping procedure was considered one CBD cycle. The amount of PbS can be increased by repeating the cycles. Subsequently, the samples were thoroughly washed with deionized water and then dried at room temperature. MEH-PPV in chloroform (20 mg/ml) was spin-coated onto the surface of the PbS QD/ZnO nanorod structures at 2,000 r/min. Films were baked in a vacuum oven for 30 min at 100°C. Then, a thin layer of poly(3,4-ethylenedioxythiophene)-poly(styrenesulfonate) (PEDOT:PSS) was spin-coated on the MEH-PPV film at 2,000 r/min and baked in a vacuum oven for 1 h at 120°C. Finally, Au was evaporated onto the device as the top electrode. The field emission scanning electron microscopy [FESEM] measurements were performed by the Hitachi FESEM S-4800 (Hitachi, Ltd., Chiyoda, Tokyo, Japan). The absorption spectrum was recorded using a Shimadzu UV-3101PC spectrophotometer (Shimadzu Corporation, Nakagyo-ku, Kyoto, Japan). Current-voltage [I-V] characteristics of the devices were measured using a Keithley 2400 SourceMeter (Keithley Instruments Inc., Cleveland, OH, USA) connected with a GPIB controller to a computer under dark or one sun illumination (AM1.5, 100 mW/cm2). All the measurements were carried out at room temperature under ambient conditions.
Figure 1 shows the typical FESEM images of ZnO nanorod arrays on an ITO glass substrate and PbS QD-coated ZnO nanorod arrays with different CBD cycles. It can be observed that the diameters of the PbS QDs are enlarged with the increasing CBD cycles. The surface of the ZnO nanorods was partially coated with the PbS QDs (Figure 1b,c) with 2 and 4 CBD cycles. However, almost the whole surface of the ZnO nanorods was coated with the PbS QDs (Figure 1d) with 6 CBD cycles, and the PbS QDs were arranged closely to each other.
Figure 2 shows the absorption spectra of ZnO nanorods, PbS QD-coated ZnO nanorod arrays with different CBD cycles, and MEH-PPV. As shown in the figure, the ZnO nanorods only absorb the high energy light with a wavelength shorter than 370 nm. With the PbS coating, the UV optical absorption edges of ZnO/PbS hybrid nanostructures are red-shifted to the long-wavelength side gradually with increasing CBD growth cycles. The absorption for the visible region is also increased a lot, ascribing to the narrow bandgap of PbS. A strong increase in absorption after each step can be observed, suggesting an increase in the number of quantum dots as well as a bathochromic spectral shift. This effect can be explained by an increase in the size after each deposition step in terms of the size quantization effect. On the other hand, the MEH-PPV showed a predominant absorption band at 400 to 570 nm.
The device structure and band diagram of the PbS  QD-sensitized MEH-PPV/ZnO  solar cells with a cascade energy alignment were shown in Figure 3. Figure 4 shows the I-V characteristics of the MEH-PPV/ZnO solar cell and the solar cells sensitized by the PbS QDs under one sun illumination (AM1.5, 100 mW/cm2) and the dark current of the PbS QD-sensitized solar cell with 4 CBD cycles. Detail parameters of the solar cells extracted from the I-V characteristics were listed in Table 1. The MEH-PPV/ZnO solar cell shows a short-circuit current density [JSC], an open-circuit voltage [VOC], a fill factor [FF], and a ηP of 1.06 mA/cm2, 0.25 V, 0.30, and 0.09%, respectively. The JSC of the PbS QD-sensitized solar cells increased with the CBD cycles, and a maximum JSC of 2.68 mA/cm2 was obtained with 4 CBD cycles. The enhancement of the JSC in the device should be due to the enhancement in absorption of the increasing PbS in Figure 2[14,21]. Meanwhile, the VOC of the PbS QD-sensitized solar cells increases monotonically with the CBD cycles, and a maximum VOC of 0.59 V is found with 6 CBD cycles. However, the FF did not show much difference with different CBD cycles. As a result, the PbS QD-sensitized solar cell with 4 CBD cycles shows a maximum ηP of 0.42%, which was increased almost five times compared with the one without PbS QDs.
The VOC was reported to track the energy difference between the highest occupied molecular orbital level of the donor and the lowest unoccupied molecular orbital level of the conduction band edge of the acceptor [5,22]. From the band diagram in Figure 3, the VOC increase in the PbS QD-sensitized MEH-PPV/ZnO solar cells can be reasonably understood because the conduction band of PbS is higher (lower electron affinity) than that of ZnO. Besides, the passivation of the surface states of the ZnO nanorods by the PbS coating led to the decreased recombination or charge trapping, and the cascade structure formed a charge carrier recombination barrier which could result in VOC improvement.
By measuring devices with different cycles of coatings, it can be seen that an optimum performance of the cell exists. The enhancement of JSC can be attributed to the cascade band structure formed with the PbS QD coating and to the higher carrier mobility in inorganic semiconductors. Such a cascade structure ensures that excitons formed in any of the three materials, e.g., ZnO nanorods, PbS QDs, and MEH-PPV, could be dissociated into a free electron and hole at the ZnO/PbS and PbS/MEH-PPV interfaces. Then, the electrons and holes will transport through ZnO and MEH-PPV to the ITO and Au electrodes, respectively. The cascade structure will restrict electron and hole recombination when transporting in the active layers and hence leads to a high charge carrier extraction efficiency. Moreover, the ZnO seed layer would avoid the direct contact between MEH-PPV and the ITO electrode and forbid the hole leakage to the ITO electrode. These factors, combining with the high VOC, bring a high ηP of 0.42% in the 4 CBD cycles of the PbS QD-sensitized MEH-PPV/ZnO solar cell. When the CBD cycles further increases, JSC decreases. The decrease of JSC with the increasing CBD cycles is considerably attributed to two reasons: one is the decrease of ZnO amount due to the growth of PbS QDs which is an erosive process  for the ZnO nanorods, and the other is ascribed to the interface restriction for the carrier transfer process between QDs. With increasing quantum of QDs, the resistance originating from the interface would become more and more dominant in the devices. For large clusters, the band alignment at the ZnO/PbS interface appears to be unfavorable for carrier transfer due to the fact that the PbS QDs are electrically isolated from each other , which result in the decrease of the JSC values. Besides, the PbS QDs may limit the MEH-PPV infiltrate into the ZnO nanorod arrays. Because of the above effects, the exciton dissociation and charge carriers transfer efficiencies could be decreased, resulting in the reduction of the ηP. Hence, the ηP of most solar cells [13,24] with PbS QDs are not high although the PbS QDs have the wider absorption compared to other QDs. It indicates that it is possible to obtain high-efficiency hybrid solar cells using suitable QDs.
In summary, an efficient PbS QD-sensitized MEH-PPV/ZnO nanorod hybrid solar cell was demonstrated. The 4 cycles of the PbS QD-sensitized solar cell showed a maximum ηP of 0.42% under one sun illumination (AM1.5, 100 mW/cm2). The improved efficiency was attributed to the cascade structure formed by the PbS QD coating, which was unfavorable for carrier transfer after redundant coating. It was expected that by using the suitable nanostructures and QDs, the efficiency of the solar cells could be further improved.
The authors declare that they have no competing interests.
LW participated in the design of the study, carried out the experiments, collected data, performed data analysis, and drafted the manuscript. DZ and ZS participated in the design of the study and helped draft the manuscript. DS conceived the study, participated in its design, and helped draft the manuscript. All authors read and approved the final manuscript.
This work is supported by the National Basic Research Program of China (973 Program) under Grant No. 2011CB302004 and by the National Natural Science Foundation of China under Grant No. 60506014 and 11004187.
|Beek WJ,Sloff LH,Wienk MM,Kroon JM,Janssen RA,Hybrid solar cells using a zinc oxide precursor and a conjugated polymerAdv Func MaterYear: 2005151703170710.1002/adfm.200500201|
|Beek WJ,Wienk MM,Janssen RA,Efficient hybrid solar cells from zinc oxide nanoparticles and a conjugated polymerAdv MaterYear: 2004161009101310.1002/adma.200306659|
|Lee YJ,Lo YS,Highly efficient quantum-dot-sensitized solar cell based on co-sensitization of CdS/CdSeAdv Func MaterYear: 20091960460910.1002/adfm.200800940|
|Lao CS,Park MC,Kuang Q,Deng Y,Sood AK,Polla DL,Wang ZL,Giant enhancement in UV response of ZnO nanobelts by polymer surface-functionalizationJ Am Chem SocYear: 2007129120961209710.1021/ja075249w17880088|
|Huang MH,Mao S,Feick H,Yan H,Wu Y,Kind H,Weber E,Russo R,Yang PD,Room-temperature ultraviolet nanowire nanolasersScienceYear: 20012921897189910.1126/science.106036711397941|
|Krebs FC,Thomann Y,Thomann R,Andreasen JW,A simple nanostrutured polymer/ZnO hybrid solar cell-preparation and operation in airNanotechnologyYear: 20081942401343402510.1088/0957-4484/19/42/42401321832673|
|Ravirajan P,Peiro AM,Nazeeruddin MK,Graetzel M,Bradley DD,Durrant JR,Nelson J,Hybrid polymer/zinc oxide photovoltaic devices with vertically oriented ZnO nanorods and an amphiphilic molecular interface layerJ Phys Chem BYear: 20061107635763910.1021/jp057137216610853|
|Peter LM,Riley DJ,Tull EJ,Wijayantha KG,Photosensitization of nanocrystalline TiO2 by self-assembled layers of CdS quantum dotsChem CommunYear: 20021010301031|
|Lin SC,Lee YL,Chang CH,Shen YJ,Yang YM,Quantum-dot-sensitized solar cells: assembly of CdS-quantum-dots coupling techniques of self-assembled monolayer and chemical bath depositionAppl Phys LettYear: 20079014351710.1063/1.2721373|
|Lee HJ,Leventis HC,Moon SJ,Chen P,Ito S,Haque SA,Torres T,Nuesch F,Geiger T,Zakeeruddin SM,Gratzel M,Nazeeruddin MK,PbS and CdS quantum dot-sensitized solid-state solar cells: "old concepts, new results"Adv Func MaterYear: 2009192735274210.1002/adfm.200900081|
|Robel I,Subramanian V,Kuno M,Kamat PV,Quantum dot solar cells. Harvesting light energy with CdSe nanocrystals molecularly linked to mesoscopic TiO2 filmsJ Am Chem SocYear: 20061282385239310.1021/ja056494n16478194|
|Bang JH,Kamat PV,Quantum dot sensitized solar cells. A tale of two semiconductor nanocrystals: CdSe and CdTeAcs NanoYear: 200931467147610.1021/nn900324q19435373|
|Plass R,Pelet S,Krueger J,Gratzel M,Bach U,Quantum dot sensitization of organic-inorganic hybrid solar cellsJ Phys Chem BYear: 20021067578758010.1021/jp020453l|
|Hoyer P,Konenkamp R,Photoconduction in porous TiO2 sensitized by PbS quantum dotsAppl Phys LettYear: 199466349351|
|Schaller RD,Klimov VI,High efficiency carrier multiplication in PbSe nanocrystals: implications for solar energy conversionPhys Rev LettYear: 20049218660118660515169518|
|Leschkies KS,Jacobs AG,Norris DJ,Aydil ES,Nanowire-quantum-dot solar cells and the influence of nanowire length on the charge collection efficiencyAppl Phys LettYear: 20099519310310.1063/1.3258490|
|Zaban A,Mićić OI,Gregg BA,Nozik AJ,Photosensitization of nanoporous TiO2 electrodes with InP quantum dotsLangmuirYear: 1998143153315610.1021/la9713863|
|Wang LD,Zhao DX,Su ZS,Fang F,Li BH,Zhang ZZ,Shen DZ,Wang XH,High spectrum selectivity organic/inorganic hybrid visible-blind ultraviolet photodetector based on ZnO nanorodsOrganic ElectronicsYear: 2010111318132210.1016/j.orgel.2010.04.010|
|Im SH,Chang JA,Woo Kim S,Wook Kim S,Seok SI,Near-infrared photodetection based on PbS colloidal quantum dots/organic hole conductorOrganic ElectronicsYear: 20101169669910.1016/j.orgel.2009.12.021|
|Lira-Cantu M,Krebs FC,Hybrid solar cells based on MEH-PPV and thin film semiconductor oxides (TiO2, Nb2O5, ZnO, CeO2 and CeO2-TiO2): performance improvement during long time irradiationSol Energy Mater Sol CellsYear: 2006902076208610.1016/j.solmat.2006.02.007|
|Guchhait A,Rath AK,Pal AJ,Near-IR activity of hybrid solar cells: enhancement of efficiency by dissociating excitons generated in PbS nanoparticlesAppl Phys LettYear: 20109607350510.1063/1.3292183|
|Olson DC,Shaheen SE,White MS,Mitchell WJ,Hest MF,Collins RT,Ginley DS,Band-offset engineering for enhanced open-circuit voltage in polymer-oxide hybrid solar cellsAdv Func MaterYear: 20071726426910.1002/adfm.200600215|
|Tak Y,Hong SJ,Lee JS,Yong K,Solution-based synthesis of a CdS nanoparticle/ZnO nanowire heterostructure arrayCryst Growth DesYear: 200992627263210.1021/cg801076b|
|Gunes S,Fritz KP,Neugebauer H,Scriciftci NS,Kumar S,Scholes GD,Hybrid solar cells using PbS nanoparticlesSol Energy Mater Sol CellsYear: 20079142042310.1016/j.solmat.2006.10.016|
Parameters of polymer/ZnO solar cells sensitized by various PbS quantum dots
CBD, chemical bath deposition; JSC, short-circuit current density; VOC, open-circuit voltage; FF, fill factor; ηP, power conversion efficiency.
Previous Document: Enhanced S-adenosyl-L-methionine production in Saccharomyces cerevisiae by spaceflight culture, over...
Next Document: A Double Mutant between Fission Yeast Telomerase and RecQ Helicase Is Sensitive to Thiabendazole, an...