Research Article  Open Access
Sheng Hsiung Chang, KuenFeng Lin, ChienHung Chiang, ShengHui Chen, ChunGuey Wu, "Plasmonic Structure Enhanced Exciton Generation at the Interface between the Perovskite Absorber and Copper Nanoparticles", The Scientific World Journal, vol. 2014, Article ID 128414, 6 pages, 2014. https://doi.org/10.1155/2014/128414
Plasmonic Structure Enhanced Exciton Generation at the Interface between the Perovskite Absorber and Copper Nanoparticles
Abstract
The refractive index and extinction coefficient of a triiodide perovskite absorber (TPA) were obtained by fitting the transmittance spectra of TPA/PEDOT:PSS/ITO/glass using the transfer matrix method. Cu nanoplasmonic structures were designed to enhance the exciton generation in the TPA and to simultaneously reduce the film thickness of the TPA. Excitons were effectively generated at the interface between TPA and Cu nanoparticles, as observed through the 3D finitedifference timedomain method. The exciton distribution is advantageous for the exciton dissociation and carrier transport.
1. Introduction
In recent years, mixed halide (CH_{3}NH_{3}PbI_{3−x}Cl_{x}) and triiodide (CH_{3}NH_{3}PbI_{3}) perovskite absorber (PA) based photovoltaics have been intensively investigated because a power conversion efficiency (PCE) of 15% can be achieved by solution processes under low temperatures [1, 2]. There are several factors that can explain the high PCE. The bandgap of PA is about 1.64 eV [3], which can absorb half of the sun light. The exciton diffusion length of PA is longer than 1 micrometer [4]; therefore the bilayered structure based photovoltaics are workable [1–4]. The exciton binding energy of PA is about 50 meV [5], which results in good exciton dissociation at the interface between the PA and PCBM (SpiroOMeTAD) [4]. The sharp optical absorption edge of PA corresponds to the small Urbach energy (~15 meV), which results in a high fill factor [6]. The thickness of PA has to be ~400 nm in order to efficiently absorb the incident sun light. However, a thicker PA is disadvantageous for exciton dissociation and carrier transport, limiting the photovoltaic performances in terms of shortcircuit current density and fill factor. A PCE as high as 20% can be expected by improving the fill factor [7]. The abovementioned drawbacks can be improved by using nanoplasmonic structures [8, 9]. Two degenerate transverse plasmon modes are supported by twodimensional ordered Cu nanoplasmonic structure embedded in P3HT:PCBM blended film, which has been designed to enhance the absorption of P3HT:PCBM based inverted photovoltaics by 22% in the visible range [9]. In this work, the Cu nanoplasmonic structures were used to enhance exciton generation in the triiodide perovskite absorber (TPA) while simultaneously reducing the film thickness of TPA. The transfer matrix method (TMM) was used to calculate the transmittance, reflectance, and absorptance. The 3D finitedifference timedomain (FDTD) method was used to observe the plasmonmediated exciton generation.
2. Optical Constants of Triiodide Perovskite Absorber
TPA was spincoated on top of the PEDOT:PSS/ITO/glass by a sequential deposition method [1]. Figure 1(a) presents the transmittance spectrum of the TPA/PEDOT:PSS/ITO/glass. The transmittance spectrum was measured by a high accuracy spectrometer (Hitachi U4100). The film thickness for each layer was measured by an step device (Veeco Dektak 150). The thicknesses of the TPA, PEDOT:PSS, and ITO were found to be 400 nm, 20 nm, and 250 nm, respectively. The refractive indices and extinction coefficients of the PEDOT:PSS thin film and the ITO film were taken from [9]. A Lorentz model was used to describe the dielectric constant of TPA, which can be written as follows: where (=1.5) is the background dielectric constant, is the th Lorentz pole, is the strength, is the oscillation frequency, and is the decay rate. Fourteen Lorentz oscillators were used in the fitting process. The transmittance spectrum of the TPA/PEDOT:PSS/ITO/glass was fitted using TMM. The fourteen oscillating wavelengths “” were fixed and are listed in Table 1. , where is light speed in vacuum. The oscillation strengths and decay rates were scanned in the fitting process. An error function (EF) is defined to evaluate the accuracy between fitting and experimental curves. Consider where (red line) is the transmittance of the fitting curve and (black line) is the measured transmittance of the TPA/PEDOT:PSS/ITO/glass. The value of the error function is equal to 0.025. The refractive index “” and extinction coefficient “” of the TPA film can be obtained by . The optical constants of TPA are plotted in Figure 1(b). The fitted parameters are listed in Table 1.

(a)
(b)
3. Plasmonic Structure Enhanced Exciton Generation
Figure 2 presents the absorptance spectra of the TPA/ITO/glass, which was calculated using TMM. The absorptance of the TPA increases with an increase in thickness from 200 nm to 400 nm. In the wavelength range of 800 nm to 900 nm, the incident nearinfrared light is absorbed by the ITO film due to the free carrier absorption. In order to reduce the thickness, a Cu nanoplasmonic structure was embedded in the TPA in order to enhance the absorptance in the effective absorption range (350 nm to 760 nm). Figure 3 presents the Cu nanoplasmonic structure embedded in the TPA thin film. In this study, the period “” was fixed at 100 nm. The gap size is defined by the difference between the period and the diameter of Cu nanoparticles.
(a)
(b)
The dipolecoupling model (DCM) [10] was adopted to calculate the effective dielectric constant of Cu nanoplasmonic structure embedded in the TPA film. These nanoplasmonic structures embedded can be treated as an effective medium. The physical concept of DCM is described in [9]. The LorentzDrude model was applied to Cu to calculate the refractive index and absorption coefficient [11].
Figure 4 presents the absorptance spectra of the TPA with and without the Cu nanoplasmonic structures. There was an increase in the absorptance of the TPA with Cu nanoplasmonic structures when the gap was changed from 50 nm to 30 nm. Compared with the red dashed line (TPA thickness = 200 nm) in Figure 4, the absorptance indicated by the black line is larger because the transverse plasmonic (TP) mode enhances the absorption (exciton generation) of the TPA. Compared with the black dashed line (TPA thickness = 400 nm) in Figure 4, the absorptance indicated by the black line is smaller. The absorptance spectra of a thicker TPA film with and without Cu nanoplasmonic structures are presented in Figure 5. Compared with the black dashed line (TPA thickness = 400 nm) in Figure 5, the absorptance indicated by the black line is higher due to the TP mode enhanced absorption even though the TPA thickness (=300 nm) is thinner. The Cu nanoplasmonic structure enhanced the absorptance of TPA in the effective absorption range (350 nm–760 nm) by 1.7% while reducing the TPA thickness from 400 nm to 300 nm.
4. Exciton Distribution
The 3D FDTD method was used to calculate the electric and magnetic field distributions of the Cu nanoplasmonic structures embedded in the TPA film. 20cell perfectly matching layers were imposed at upper and lower boundaries to absorb the outgoing electromagnetic waves without producing significant reflections back into the simulation domain. The simulation of twodimensional ordered Cu nanoparticle arrays was performed using periodic boundary conditions. The cell size and the time step used in discretization of the space domain and time domain were 1 nm × 1 nm × 1 nm and 1.9 × 10^{−18} s, respectively. A planewave with an directed electric field was launched from the glass substrate along the positive direction.
Figure 6 presents the field distributions of the  plane at the resonant wavelength of TP mode. The strengths of electric field and magnetic field both increased when the gap was changed from 50 nm to 30 nm. The incident light is trapped and redistributed in space to effectively generate excitons at the interface between the TPA and Cu nanoparticles. Conceptually, the excitons can be dissociated at the interface between TPA and Cu nanoparticles because the HOMO level (−5.4 eV) [3] of the TPA is lower than the Fermi level of Cu (−4.94 eV) [12]. Therefore, the localized field distribution benefits the exciton dissociation.
(a)
(b)
(c)
(d)
(e)
(f)
Figure 7 presents the electric field distributions of Cu nanoplasmonic structures embedded in the TPA film on the  plane. The electric fields (excitons) are localized (generated) around the lower surface of Cu nanoparticles. Therefore, the excitons are dissociated mostly from the lower surface of the Cu nanoparticles. After exciton dissociation, the holes (electrons) can propagate along the Cu (TPA) to the anode (cathode) electrode. In such cases, carrier recombination can be reduced.
(a)
(b)
(c)
5. Conclusions
In conclusion, we have assessed the optical effects of Cu nanoplasmonic structure embedded in triiodide perovskite absorber (TPA). The refractive index and absorption coefficient of TPA were obtained by fitting the transmittance spectrum of TPA/PEDOT:PSS/ITO/glass using transfer matrix method. Cu nanoplasmonic structures could reduce the TPA thickness from 400 nm to 300 nm while keeping the absorption strength. The 3D finitedifference timedomain method was used to observe the distribution of the electric field (generated excitons). The electric field is redistributed at the interface between the TPA and Cu nanoparticles, which benefits the exciton dissociation and carrier transport.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgment
This work was supported by the National Science Council under Grant NSC 1012731M008002MY3.
References
 J. Burschka, N. Pellet, S.J. Moon et al., “Sequential deposition as a route to highperformance perovskitesensitized solar cells,” Nature, vol. 499, no. 7458, pp. 316–319, 2013. View at: Publisher Site  Google Scholar
 D. Liu and T. L. Kelly, “Perovskite solar cells with a planar heterojunction structure prepared using roomtemperature solution processing techniques,” Nature Photonics, vol. 8, pp. 133–138, 2014. View at: Google Scholar
 G. Xing, N. Mathews, S. Sun et al., “Longrange balanced electron and holetransport lengths in organicinorganic CH_{3}NH_{3}PbI_{3},” Science, vol. 342, pp. 344–347, 2013. View at: Google Scholar
 S. D. Stranks, G. E. Eperon, G. Grancini et al., “Electronhole diffusion lengths exceeding 1 micrometer in an organometal trihalide perovskite absorber,” Science, vol. 342, pp. 341–344, 2013. View at: Google Scholar
 V. D'Innocenzo, G. Grancini, J. P. Marcelo et al., “Excitons versus free charges in organolead trihalide perovskites,” Nature Communications, vol. 5, article 3586, 2014. View at: Publisher Site  Google Scholar
 S. de Wolf, J. Holovsky, S.J. Moon et al., “Organometallic halide perovskites: sharp optical absorption edge and its relation to photovoltaic performance,” The Journal of Physical Chemistry Letters, vol. 5, no. 6, pp. 1035–1039, 2014. View at: Publisher Site  Google Scholar
 N.G. Park, “Organometal perovskite light absorbers toward a 20% efficiency lowcost solidstate mesoscopic solar cell,” The Journal of Physical Chemistry Letters, vol. 4, no. 15, pp. 2423–2429, 2013. View at: Publisher Site  Google Scholar
 N. F. Fahim, B. Jia, Z. Shi, and M. Gu, “Simultaneous broadband light trapping and fill factor enhancement in crystalline silicon solar cells induced by Ag nanoparticles and nanoshells,” Optics Express, vol. 20, no. 19, pp. A694–A705, 2012. View at: Publisher Site  Google Scholar
 S. H. Chang, “Modeling and design of Ag, Au, and Cu nanoplasmonic structures for enhancing the absorption of P3HT:PCBMbased photovoltaics,” IEEE Photonics Journal, vol. 5, no. 3, Article ID 4800509, 2013. View at: Publisher Site  Google Scholar
 S. H. Chang, B.Y. Lin, T.Y. Cheng, and J.K. Wang, “Unraveling electromagnetic resonance of twodimensional ordered nanoparticle arrays with a dipolecoupling model,” Physica Status Solidi: Rapid Research Letters, vol. 4, no. 10, pp. 259–261, 2010. View at: Publisher Site  Google Scholar
 A. D. Rakić, A. B. Djurišić, J. M. Elazar, and M. L. Majewski, “Optical properties of metallic films for verticalcavity optoelectronic devices,” Applied Optics, vol. 37, no. 22, pp. 5271–5283, 1998. View at: Publisher Site  Google Scholar
 P. O. Gartland, S. Berge, and B. J. Slagsvold, “Photoelectric work function of a copper single crystal for the (100), (110), (111), and (112) faces,” Physical Review Letters, vol. 28, no. 12, pp. 738–739, 1972. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2014 Sheng Hsiung Chang 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.