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完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor陳俊維
dc.contributor.authorYing-Chiao Wangen
dc.contributor.author王映樵zh_TW
dc.date.accessioned2021-06-15T16:09:38Z-
dc.date.available2020-08-25
dc.date.copyright2015-08-25
dc.date.issued2015
dc.date.submitted2015-08-18
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/52212-
dc.description.abstract本研究利用材料之特殊性質以獲得低成本與高效率之染料敏化太陽能電池。然而,染敏元件發展近二十年來,其光電轉換效率仍無法有效提升至可商業化的程度。所以,尋找更適合的吸光材料,便成為下一個重要課題。近年來,鈣鈦礦材料因同時具備多種成為光學主動層的優點,使得其元件效能可劇烈的提升至19%。其中,鈣鈦礦的結晶轉化程度更是決定元件效能的重要關鍵,本論文將探討元件中鈣鈦礦晶體的結晶型態。進一步,我們亦將引入奈米晶體添加劑提升鈣鈦礦材料的光電特性,以提供未來研究高效能之鈣鈦礦太陽能電池的依據。
第一部分,首先使用二硫化鐵(FeS2),別名黃鐵礦。因為黃鐵礦的色澤呈閃閃發亮的金黃色,經常被誤認為是黃金,故俗稱『愚人金』。由於二硫化鐵在地球中含量豐沛、無毒且為低能帶隙的礦材,因此被科學家廣泛討論並視為下一世代有趣的光電材料之一。使用溶液旋轉塗佈法可製備溶膠狀之二硫化鐵奈米晶體,此低廉之奈米顆粒提供很大的潛力以發展二硫化鐵為基底的光伏打元件。近日,我們使用黃鐵礦奈米墨液來製作的光伏打應用設備。這個原料無毒且在大自然更容易取得,不僅能製造出更有經濟效益的對電極,亦能取代在染料敏化太陽能電池中較貴的白金電極。黃鐵礦奈米晶體也展現了非常好的電化學催化活性以及電化學穩定度。另外,以此室溫塗佈法來製備二硫化鐵對電極可應用於軟性基板(PET-ITO);且因為二硫化鐵對電極呈現半透明,可在背面照光下得到比白金對電極更優越的元件效能。這項研究使得低成本的黃鐵礦二硫化物奈米晶體催化作用於染料敏化太陽能電池及其它電化學電池的相關應用更為清楚明顯。
再者,離子擴散速率差異導致再生染劑的障礙及工作電極/電解液界面的載子再結合現象為染料敏化太陽能電池中能量損耗的一大因素。一般而言,文獻上會以超薄的無機電子阻隔層以達到改善之目的。然而,這些表面覆蓋物會導致染料吸附量下降與阻礙電解液還原染料的機率。因此,我們利用溶液塗佈一具備雙功能之有機共聚物Poly (vinylidene fluoride-trifluoroethylene) (P(VDF-TrFE))於含有染料之工作電極上。經修飾過後的工作電極除了有減少電子電洞再結合的功能,更因為P(VDF-TrFE)具備優良的導離性,而促進離子的擴散,進一步增進染料的再生機會。利用此簡易製程之廉價共聚物改善後的元件更因此提升了18.7%的元件效能。
第三部分,在有機無機混成鈣鈦礦組成太陽能電池的領域,因為光電轉換效率快速的躍進,迅速成為下一世代低成本太陽能電池具有潛力的吸光層。然而,高度結晶化的鈣鈦礦才能夠提供更高的吸光效能與形成更有效的載子傳輸媒介。在此,我們利用逐步沉積的技術來控制鈣鈦礦的晶體轉化率。過程中,利用XRD與XPS儀器監測,我們可以獲知PbI2與甲胺碘中解離出來的碘離子形成[PbI6]4-八面體。隨著甲胺碘含量增加,八面體成長為鈣鈦礦之tetragonal結構。晶體完整時,為了降低能量,甲胺陽離子會進入tetragonal的interstitial 位置內,並藉此達到高吸光能力的材料。由於,XRD只能看到tetragonal結構成型的情況,若能搭配XRD 縱深分析與二維GIXRD的綜合探討,可以獲知不同轉化率鈣鈦礦晶體之分布情形,更進一步可推斷初始之PbI2晶體排列將直接影響鈣鈦礦材料的晶體方向,日後亦更可精確控制鈣鈦礦的成長,與有效掌握元件之效能。
第四部分,我們利用化學方法置換二氧化鈦奈米柱之配體,因此在室溫下,鈣鈦礦前驅物即可均勻分散二氧化鈦奈米柱。反應後,可形成塊材混參之結構。此嶄新鈣鈦礦/二氧化鈦奈米柱塊材混參太陽能電池之光電轉換效率可達到12%。此一混參概念,除可提供溫度敏感型基板之應用,亦可引入工業製程以提供未來鈣鈦礦多層複雜結構之製備。
最後,我們將硫化鉛奈米晶體之配體以碘離子置換,用以混入鈣鈦礦前驅物溶液中,並進而改變鈣鈦礦材料的結晶行為。結晶過程中,硫化鉛奈米晶體表面的碘離子配體將與鈣鈦礦前驅物形成螯合反應。由於活化能的降低,鈣鈦礦晶體的反應性將被大幅提升。鈣鈦礦/碘離子配體亦將形成新的集中型晶種,成長時,鈣鈦礦晶體將有較大的成長空間。此一大晶粒之鈣鈦礦平面結構型太陽能電池存在高達76.3%之填充因子與16%之光電轉換效率。此大晶粒之鈣鈦礦使載子傳輸性質提升。為了瞭解晶粒大小與載子傳輸性質之關係,本研究利用時間解析光致螢光與雙極性載子傳輸方程式來分析鈣鈦礦材料的載子擴散長度。結果發現,因為大晶粒的鈣鈦礦單位長度內的晶粒邊界較少,使得載子在其中得以更加順利的擴散至電極,所以具有較長的電子與電洞擴散長度。根據此研究結果,未來可以經由設計適合之奈米晶種,以提升鈣鈦礦之材料性質與提高元件效率。
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dc.description.abstractFirst, we present the colloidal pyrite FeS2 nanocrystals (NCs), which are abundant in nature and nontoxic, have attracted attention for developing low-cost fabrications of photovoltaic (PV) devices using solution processes. This section demonstrates an important PV application using FeS2 nanocrystal pyrite ink to fabricate a cost-effective counter electrode (CE) to replace the expensive Pt counterpart in dye-sensitized solar cells (DSSCs). FeS2 NC ink has exhibited excellent electrochemical catalytic activity and remarkable stability and showed a promising power conversion efficiency (PCE) comparable to that using a Pt CE. Solution-processable and semitransparent FeS2 NC-based CEs also enable the fabrication of flexible and bifacial DSSCs. The results indicate that earth-abundant FeS2 NC ink is an extremely interesting candidate for replacing the precious metal of Pt for employing the iodide/triiodide redox couples, which can substantially lower the cost of DSSCs in future commercial applications.
Next, the impedance of interception of the oxidized dye (S+) by electron donors in the electrolyte, and recombination of the electron in the dye-adsorbed mesoporous electrode with S+ or electrolyte species have been identified as the main cause of energy loss in DSSCs. Generally, an ultrathin inorganic electron blocking material surrounding working metal oxides is required to inhibit their recombination and further promoted electron-transfer reactions. However, the surface passivation interlayers would decrease adsorption of the dye resulting in reduces the interface between the dye molecules and semiconductors or decreases the quantum efficiency for electron injection, which all led to a reduced photocurrent. Here, we demonstrate an important PV application using a dual functional poly (vinylidene fluoride-trifluoroethylene) (P(VDF-TrFE)) copolymer deposited onto the dye penetrant working electrode (WE) by a solution-processed method. The WE after introduced the conformal P(VDF-TrFE) interlayer have both ability of reducing carrier recombination and facilitating ionic mobility, therefore, the further enhancement of 18.7% PCE in DSSCs. These results indicate that the cost-effective P(VDF-TrFE) copolymer is an extremely interesting candidate for promoted dual functions of electron collection efficiency and S+ regeneration rate, which can substantially higher the efficiency of DSSCs in future commercial applications.
In Chapter 5, organometal halide perovskite materials were identified as promising light harvesters to achieve rapidly boosted performance, providing great potential for developing low-cost next-generation photovoltaic devices. The highly crystalline perovskite is required either to absorb most of the sunlight or deliver efficient charge transport pathways for photogenerated carriers. Here, we use a sequential deposition technique for prepared perovskite crystals under various conversion ratios to demonstrate the mechanisms of an extended three-dimensional network of corner-sharing [PbI6]4- octahedral and then filled the methylammonium (MA) to 12-fold iodide coordinated interstitial sites among the octahedral by X-ray diffraction (XRD) spectrum and X-ray photoelectron spectroscopy (XPS), respectively, during crystal growth. Furthermore, the vertical distributions of morphology and crystal structure have important implication for analyzed depth profile of the perovskite structures using the XRD depth profiles and two-dimensional GIXRD spectra measurement. These results indicate that through clearly realized material engineering, and the most significant differences in efficiency are attributed to whether enhances transformation of perovskite by the orderly built the inorganic frameworks and completely inserted the organic molecules.
Furthermore, to replace high-temperature sintered scaffold materials in conventional CH3NH3PbI3-based solar cells, this study demonstrates a new device structure of a bulk intermixing (BI)-typed CH3NH3PbI3/TiO2 nanorods (NRs) hybrid solar cell, where dispersed TiO2 NRs from chemical synthesis are intermixed with the perovskite absorbing layer to form a BI-typed perovskite/TiO2 NRs hybrid for device fabrication. Through interface engineering between TiO2 NR surface and the photoactive perovskite material of CH3NH3PbI3 by ligand exchange treatment, a remarkable power conversion efficiency (PCE) of over 12% was achieved based on the simple BI-typed CH3NH3PbI3/TiO2 NR hybrid device structure. The proposed hybrids not only provide great flexibility for deposition on various substrates through spin coating at low temperatures but also enable layer-by-layer deposition for future development of perovskite-based multi-junction solar cells.
Finally, the utilization of iodide ligand assisted lead sulfide nanocrystal (PbS/I-) as the seeds for heterogeneous-nucleation in perovskite solar cells is demonstrated. Through interface engineering between PbS nanocrystal surface and the perovskite material of CH3NH3PbI3Cl3-x as a result of improvement crystallinity of the perovskite film and further formed large grain sized morphology by ligand exchange treatment, a remarkable power conversion efficiency of 16% was achieved. Both electron and hole diffusion length of large grain perovskite are longer than the pristine sample, indicated that the smaller trap densities in the large grain sized perovskite crystals. Therefore reduced charge transfer resistance across the perovskite material that growth from PbS/I-, so that achieved the higher fill factor and short circuit current density. Our results indicate that PbS nanocrystal could be a simple solution-processable introducing to perovskite precursor solution as the nuclei and multidentate chelation ligands in perovskite solar cells.
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dc.description.tableofcontentsTOC II
謝 誌 V
摘 要 VII
Abstract XI
Table of Contents XV
Figure Index XXI
Table Index XXX
Chapter 1 1
Introduction 1
1.1 Sun, energy and solar cells 1
1.2 Dye-sensitized solar cells 3
1.3 Challenges in dye-sensitized solar cells 6
1.4 Perovskite solar cells 7
1.5 Outline of this thesis 12
1.6 References 17
Chapter 2 19
Experimental 19
2.1 Photovoltaic characteristics 19
2.1.1 Solar spectrum 19
2.1.2 I-V characteristic of the photovoltaic devices 20
2.1.3 Incident photon to current conversion efficiency (IPCE) 23
2.2 Electrochemical systems 24
2.2.1 Oxidation/Reduction (Redox) reactions 24
2.2.2 Mechanisms of catalysis 25
2.2.3 Electrochemical polarization and Tafel curve 26
2.2.4 Cyclic voltammetry 31
2.3 Photocarrier dynamic measurements 32
2.4 X-ray photoelectron spectroscopy (XPS) 33
2.4.1 X-ray photoelectron spectroscopy principles 33
2.4.2 Spin-orbit coupling effects 35
2.4.3 Chemical shifts 36
2.5 References 38
Chapter 3 39
Progress in Dye-Sensitized Solar Cells 39
3.1 Photoelectrochemical cells for solar energy conversion 39
3.2 Photochemistry of semiconductor-liquid junctions 39
3.3 Principles of dye-sensitized solar cells 42
3.3.1 Mechanisms 42
3.3.2 Photovoltage 43
3.3.3 Electron injection 45
3.3.4 Dye regeneration 47
3.3.5 Electron loss or recombination 48
3.4 Progress in study each parts of dye-sensitized solar cells 49
3.4.1 The photoactivers 49
3.4.2 The electrolytes 54
3.4.3 The catalytic electrodes 57
3.4.4 The working electrodes 59
3.5 References 63
Chapter 4 67
FeS2 Nanocrystal Ink as a Catalytic Electrode for Dye-Sensitized Solar Cells* 67
4.1 Introduction 67
4.2 Experimental section 70
4.2.1 Preparation of FeS2 counter electrodes 70
4.2.2 Fabrication of the dye-sensitized solar cell 71
4.2.3 Characterizations and measurements 72
4.3 Preparation of FeS2 nanocrystals and its ligand exchange effect 73
4.4 Device performance with various counter electrodes 75
4.5 Electrochemical activity of FeS2 counter electrodes 77
4.6 Using first-principles to predict the reduction reaction by FeS2 82
4.7 FeS2 counter electrode application in flexible substrate and bifacial dye-sensitized solar cells 84
4.8 Summary 87
4.9 References 88
Chapter 5 91
Enhanced Efficiency in Dye-Sensitized Solar Cells with a Dual Functional Polymer Interlayer for Facilitating Ionic Diffusion and Reducing Carrier Recombination 91
5.1 Introduction 91
5.2 Experimental section 95
5.2.1 Preparation of P(VDF-TrFE) working electrodes 95
5.2.2 Fabrication of the dye-sensitized solar cell 96
5.2.3 Characterizations and measurements 97
5.3 Modified the working electrode architecture through conformal coating P(VDF-TrFE) copolymer 98
5.4 Energy band alignment and electronic property of P(VDF-TrFE) 101
5.5 Electrocatalytic behavior across a P(VDF-TrFE) interlayer 103
5.6 Dye-sensitized solar cells using P(VDF-TrFE) as a dual functional matrix for facilitating ionic diffusion and reducing carrier recombination 107
5.7 Charge-collection efficiency improvement 111
5.8 Summary 114
5.9 References 115
Chapter 6 119
Progress in Perovskite Solar Cells 119
6.1 Growth mechanism of the origanic-inorganic perovskite material 119
6.1.1 Two-dimensional layered organic-inorganic perovskites 119
6.1.2 Three-dimensional cubic organic-inorganic perovskites 121
6.2 Photocarrier dynamics in perovskite solar cells 122
6.3 Device architectures of perovskite solar cells 125
6.3.1 Mesoporous structure 125
6.3.2 Mesoporous structure with nonelectron injecting oxides 126
6.3.3 Planar structure 127
6.3.4 Hybrid structure 129
6.4 References 132
Chapter 7 135
Vertical Composition and Morphology Analysis of High Performance Perovskite Solar Cells 135
7.1 Introduction 135
7.2 Experimental section 138
7.2.1 CH3NH3I preparation 138
7.2.2 Fabrication of the perovskite solar cells 138
7.2.3 Characterizations and measurements 139
7.3 Performance of perovskite solar cells treated with various amounts of methylamine iodide based precursor 140
7.4 Morphology evolution of perovskite materials during different conversion ratios 145
7.5 Crystallinity and chemical composition analyses of perovskite crystals in the devices 148
7.6 Vertical profiles of perovskite crystals in the devices 153
7.7 Summary 160
7.8 References 161
Chapter 8 163
Bulk Intermixing-Typed Perovskite CH3NH3PbI3/TiO2 Nanorod Hybrid Solar Cells 163
8.1 Introduction 163
8.2 Experimental section 166
8.2.1 Synthesis of TiO2 nanorods 166
8.2.2 Ligand exchange process 167
8.2.3 Fabrications of BI- typed perovskite solar cells 168
8.2.4 Characterizations and measurements 169
8.3 Material perporty in a BI-type CH3NH3PbI3/TiO2 NRs hybrid perovskite solar cell 170
8.4 Nanoscale morphology of the perovskite/TiO2 NRs hybrid 173
8.5 Ligand exchange effect 176
8.6 Inference of the concentrations of TiO2 NR in the BI devices 181
8.7 Summary 186
8.8 References 187
Chapter 9 189
Nanocrystals Assisted Heterogeneous-Nucleation at Grain Growth of High-Performance Perovskite Solar Cells 189
9.1 Introduction 189
9.2 Experimental sectional 192
9.2.1 Synthesis of PbS nanocrystals 192
9.2.2 Ligand exchange process 192
9.2.3 Fabrications of the PbS/I- modified perovskite solar cell 193
9.2.4 Characterizations and measurements 194
9.3 Formed Polar PbS nanocrystals after ligand exchange treatments 195
9.4 Perovskite with large grain size and highly crystallinity after introducting PbS/I- nuclei 199
9.5 Photovoltaic performance of PbS/I- based perovskite solar cells 202
9.6 Longer diffusion length exhibited in PbS/I- based perovskite solar cells 206
9.7 Summary 209
9.8 References 210
Chapter 10 213
Curriculum Vitae 213
10.1 Self Introduction 213
10.2 Education 213
10.3 List of Publications 213

Figure Index
Figure 1.1 (a) DSSC device schematic and operation. (b) Energy level and device operation of DSSCs.9 5
Figure 1.2 The nanocrystalline effect in dye-sensitized solar cells. The incident photon to current conversion efficiency (IPCE) is plotted as a function of the excitation wavelength. (a) Single-crystal anatase cut in the (101) plane. (b) Nanocrystalline anatase film.3 5
Figure 1.3 The model of the basic perovskite structure.22 9
Figure 1.4 IPCE spectra for solar cells sensitized by various perovskite materials (right).23 11
Figure 1.5 Energy level diagram of TiO2, perovskite, and spiro-MeOTAD.25 11
Figure 1.6 (a) HR-TEM image, (b) FeS2 NCs ink and (c) current density-voltage (J-V) characteristics of the DSSCs, measured under AM 1.5 illumination. The inset figure shows the corresponding FeS2 NCs thin film on the ITO glass. 12
Figure 1.7 A schematic illustration of P(VDF-TrFE) copolymer coated WE in a DSSC. 13
Figure 1.8 Chemical composition and vertical profile of the CH3NH3PbI3 crystal applied in the photovoltaic device. 14
Figure 1.9 Device architecture of a bulk intermixing(BI)-typed perovskite solar cell and the TEM image of TiO2 nanorods. 15
Figure 1.10 PbS nanocrystals assisted heterogeneous-nucleation at grain growth of perovskite solar cells. 16
Figure 2.1 Current vs. voltage characteristic of a solar cell under illumination and in the dark. The marks of (a), (b), (c) and (d) indicated the conditions at Jsc, Voc, reverse and forward bias, respectively.4 22
Figure 2.2 Metal-semiconductor-metal of organic diode devices. At the four conditions of (a) zero bias (b) Voc, (c) reverse bias and (d) forward bias.4 23
Figure 2.3 Mechanisms of catalytic reaction.5 26
Figure 2.4 Illustration of electrical double layer.6 27
Figure 2.5 Regions of a polarization curve. 29
Figure 2.6 A typical Tafel curve and the corresponding electrochemical parameters. 30
Figure 2.7 (a) A triangular potential waveform with switching potentials and (b) the corresponding cyclic voltammogram.7, 8 32
Figure 2.8 The process of photoionization. 35
Figure 2.9 XPS spectrum at Pb 4f core level of PbI2 film. 36
Figure 2.10 Chemical shifts between the PbI2 and CH3NH3PbI3 films at XPS Pb 4f core level. 37
Figure 3.1 The three known methods by which solar energy can be converted into usable chemical and/or electrical energy.1 41
Figure 3.2 Binding model of carboxylate unit on the metal oxide surface.34 50
Figure 3.3 UV-Vis absorption spectrum of N719 dye. Inset: the structure of N719.35 51
Figure 3.4 Interfacial electron transfer involving a ruthenium complex bound to the surface of TiO2 via a carboxylated bipyridyl ligand.2 52
Figure 3.5 Overview of processes and typical time constants under 1 sun in a Ru–dye–sensitized solar cell with iodide/triiodide electrolyte. Recombination processes are indicated by red arrows.34 52
Figure 3.6 Design principle of an organic dye for TiO2 photoanodes in DSSCs.36 54
Figure 3.7 Band diagrams of semiconductors with respect to several redox couples.50 59
Figure 4.1 XRD spectra of FeS2 NC thin films. 74
Figure 4.2 (a) HR-TEM image and (b) fast Fourier transform (FFT) pattern of FeS2 NCs. The photograph images of (c) FeS2 NCs ink and (d) the FeS2 NCs thin film as a CE on the ITO glass. (e) Top and (f) cross-sectional scanning electron microscopy (SEM) images of the densely packed FeS2 NC thin film on the ITO glass. 75
Figure 4.3 Current density-voltage (J-V) characteristics of the DSSCs with Pt-CE and FeS2-CEs (with and without EDT treatment), measured in the dark and under AM 1.5 illumination (100 mW cm-2 ). 76
Figure 4.4 (a) Cyclic voltammograms (CVs) of Pt-CE, FeS2-CEs with and without EDT treatment, in 10 mM LiI, 1 mM I2, and 0.1 M LiClO4 in ACN, at a scan rate of 50 mV s-1. (b) 500 consecutive CVs of the FeS2-CE with EDT treatment at a scan rate of 50 mV s-1. The inset shows the anodic and cathodic peak current densities vs. cycle times. 78
Figure 4.5 (a) Nyquist plots of the symmetrical cells based on Pt-CE and FeS2-CEs with and without EDT treatment and (b) Tafel polarization curves at the scan rate of 50 mV s-1 based on the same devices in (a). 81
Figure 4.6 Flatted AFM images of (a) of Pt-CE, FeS2-CE (b) with and (c) without EDT treatment, and 3D AFM images of (d) of Pt-CE, FeS2-CE (e) with and (f) without EDT treatment. 81
Figure 4.7 (a) Adsorption sites of on and the optimized structures in the (b) atop (c) bridge configurations. 84
Figure 4.8 (a) PDOS of iodine and iron atoms in the system. (b) The slicing contour plot of the bonding state of in the atop configuration. 84
Figure 4.9 Current density-voltage (J-V) characteristics of the DSSC using the FeS2-CE deposited on ITO/PET substrate, measured in the dark and under 100 mW cm-2 illumination. 85
Figure 4.10 Current density-voltage (J-V) characteristics of the DSSCs consisting of the reference Pt-CE and semi-transparent FeS2-CE under rear illumination (100 mW cm-2). The inset figure shows the corresponding transmittance of Pt-CE and FeS2-CE. 87
Figure 5.1 The structure of poly (vinylidene fluoride-trifluoroethylene) (P(VDF-TrFE)) copolymer. 95
Figure 5.2 (a) TEM image of a P(VDF-TrFE) coated TiO2 nanoparticle. Scanning TEM energy dispersive X-ray spectra (EDS) mappping of the (b) carbon, (c) titanium concentrations and (d) it’s composite in the nanoparticle of (a). 99
Figure 5.3 TEM image of a TiO2 nanoparticle after annealed at 450 oC for 30 min. 100
Figure 5.5 FE-SEM of (a) top and (b) cross sectional views of TiO2, (c) top and (d) cross sectional views of TiO2/dye, and (e) top and (f) cross sectional views of TiO2/dye/P(VDF-TrFE), respectively. 101
Figure 5.6 (a) Cyclic voltammetry (CV) graph and (b) absorption spectrum of P(VDF-TrFE) copolymer. (c) The corresponding energy levels of the device. (d) Conductive-AFM (C-AFM) current-voltage characteristics of P(VDF-TrFE) consisting of various thickness. Inset plots of (a) CV of ferrocene is shown for the calibration, (b) Tauc plots of P(VDF-TrFE) showing possible fits to obtain the band gap and (d) schematic of the structure to measured C-AFM. 103
Figure 5.7 Steady-state voltammograms corresponding to with and without P(VDF-TrFE) coated WEs using the electrochemical devices of WE/electrolyte/Pt-CE in the dark. Scan rate: 50 mV s-1. 106
Figure 5.8 Steady-state voltammograms corresponding to various WEs based electrochemical devices (WE/electrolyte/Pt-CE) under AM 1.5 illumination of 100 mW cm-2. Scan rate: 50 mV s-1. 106
Figure 5.9 (a) Current density-voltage (J-V) characteristics measured in the dark and under AM 1.5 illumination of 100 mW cm-2. (b) Incident photon-to-electron conversion efficiencies (IPCEs), (c) Nyquist plots (frequency scan range was set from 1MHz to 10 mHz) and (d) Bode phase diagrams at AM 1.5 illumination (100 mW cm-2 ) of the DSSC devices with and without P(VDF-TrFE) coated WEs. 110
Figure 5.10 (a) Charge transit time versus short-circuit current density and (b) electron lifetime as a function of open-circuit voltage measured by IMPS and IMVS, respectively, at different light densities for the DSSC devices with and without P(VDF-TrFE) coated WEs. 113
Figure 5.11 Short-circuit current density versus light intensity measured by IMPS at different light densities for the DSSC devices without and with P(VDF-TrFE) coated WEs. 113
Figure 6.1 Schematic of 2D organic-inorganic <100>-oriented perovskite materials with (a) monoammonium and (b) diammonium cationic organic molecules.3 120
Figure 6.2 Intergrowth structures formed from the alternate arrange of 3D and 2D perovskites.3 122
Figure 6.3 Photocarrier dynamics in perovskite solar cells. The peovskite sensitizer is sandwiched between an electron transfer layer (ETL) and a hole transfer layer (HTL). From (a) to (f) indicated the photocurrent generate processes, and from (g) to (i) are energy loss reactions. 124
Figure 6.4 Solid-state device and its mesoporous structure. (a) Photography image of the device. (b) Cross-sectional scheme of the device. Cross-sectional SEM image of (c) the device and (d) perovskite/underlayer/FTO interfacial junction structure.22 126
Figure 6.5 Schematic illustrating the charge migrate in a TiO2 based perovskite solar cell (left), a noninjecting Al2O3 based perovskite solar cell (right). The band duagram is shown below accompanied with electrons (solid circles) and holes (open circles).23 127
Figure 6.6 SEM top views of (a) a vapour-deposited perovskite film and (b) a solution-processed perovskite film. Cross-sectional SEM images under high magnification of complete solar cells constructed from (c) a vapour-deposited perovskite film and (d) a solution-processed perovskite film. Cross-sectional SEMimages under lower magnification of completed solar cells constructed from (e) a vapour-deposited perovskite film and (f) a solution-processed perovskite film.27 129
Figure 6.7 Schematic of the perovskite solar cell with a self-assembled monolayer of C60 fullerene functionalization.31 131
Figure 6.8 (a) Schematic of the typical full device structure, where the mesoporous oxide is either loaded with GQDs or not, (b) the band alignment, and (c) the edge-modified GQD structure. (d) Cross-sectional SEM image of a complete photovoltaic device after GQDs modified.32 131
Figure 7.1 (a) Current density-voltage (J-V) characteristics of the perovskite solar cells using perovskite photoactives reaction with different amounts of MAI precursor under AM 1.5 irradiation. (b) Incident photon-to-electron conversion efficiencies (IPCEs) of the photovoltaic devices with AM 1.5G photo flux. (c) UV-visible absorption spectra by loading various conversion ratios of perovskite material. (d) Time-resolved photoluminescence (TRPL) spectroscopy of CH3NH3PbI3/mesoporous-TiO2 layers prepared by PbI2 reaction with different concentrations of MAI solution. 144
Figure 7.2 Top-view SEM images of (a) PbI2 film and perovskite came from various concentrations of MAI: (b) 2 mg/ml; (c) 5 mg/ml; (d) 10 mg/ml; and (e) 12 mg/ml. And cross-sectional SEM images of (f) PbI2 film and perovskite obtained from various concentrations of MAI: (g) 2 mg/ml; (h) 5 mg/ml; (i) 10 mg/ml; and (j) 12 mg/ml. 147
Figure 7.3 (a) X-ray diffraction (XRD) spectra and (b) X-ray photoelectron spectroscopy (XPS) at Pb 4f core level of PbI2 film and perovskite consisted of various amounts of MAI solution. Schematic representations of (c) before and after organic CH3NH3+ created effectively hydrogen bond to the halides of extended [PbI6]4- sheets at the lower dimensional octahedral network and (d) the CH3NH3+ integrated into the interstitial sites of [PbI6]4- octahedral network by van der Waals interaction and further consisted of the 3D perovskite frameworks. 152
Figure 7.4 (a) XRD depth-profiling analysis of perovskite materials consisted of various amounts of MAI using (a) 2mg/ml; (b) 5mg/ml; and (c) 10 mg/ml at various incident angles. 155
Figure 7.5 (a) Scheme of GIXRD setup (λ = 8.2 × 10-2 nm) for in-plane and out-of-plane measurements. 2D GIXRD images of PbI2 films at incident angle of (b) 0.1 and (c) 1.2, respectively. (d) Scheme of vertical morphology and crystal orientation of PbI2 film. 157
Figure 7.6 2D GIXRD images of sample A at incident angle of (a) 0.1 and (b) 1.2, respectively. 2D GIXRD images of sample C at incident angle of (c) 0.1 and (d) 1.2, respectively. (e) Scheme of vertical morphology and crystal orientation of sample A. (e) Scheme of vertical morphology and crystal orientation of sample C. 159
Figure 8.1 TEM image of TiO2 nanorods. Inset: the corresponding high resolution image. 166
Figure 8.2 (a) Sequential deposition processes of a BI-type perovskite layer. PbI2/TiO2 hybrid solution was spun-coated in the first step and CH3NH3I solution was then drop-cast onto the PbI2/TiO2 NRs hybrid thin film in the second step to grow the CH3NH3PbI3/TiO2 NRs hybrid thin film. (b) Top-view surface morphology of the CH3NH3PbI3/TiO2 NRs intermixed hybrid layer and (c) SEM cross-section image of a BI-type CH3NH3PbI3/TiO2 NRs hybrid perovskite solar cell. 173
Figure 8.3 (a) Planar-view HAADF-STEM image of PbI2/TiO2 NRs hybrid thin film. (b)-(c) EELS elemental maps of Ti and I, respectively. (d) XPS depth profile of Ti 2p binding energy of a BI-typed CH3NH3PbI3/TiO2 NRs hybrid thin film. 176
Figure 8.4 (a) Chemical structures of surface ligands of oleic acid (OA), pyridine (PYR) and acrylic acid (ACR). (b) FTIR transmission spectra of TiO2 NRs before and after surface ligand exchange treatments. (c) TRPL spectra and the inset of (c) PL spectra of the pristine CH3NH3PbI3 and CH3NH3PbI3/TiO2 NRs hybrids with various surface ligand exchange treatments. The corresponding current-voltage curves of photovoltaic performances of these devices under AM 1.5 solar irradiation. (100mW/cm2). 180
Figure 8.5 (a) Device performances of BI-typed CH3NH3PbI3/TiO2 NRs hybrid solar cells with various ACR-capped TiO2 NRs concentrations. (b) EQE spectrum of the best-performing solar cell. The verified photocurrent density by integrating EQE spectrum is also shown. 185
Figure 8.6 Surface morphology of BI-typed perovskite films with 2.0 mg/ml of ACR-TiO2. 185
Figure 9.1 (a) TEM and insert HR-TEM images and (b) legend exchange of PbS nanocrystals. (c) FTIR transmission spectra and (d) XPS of Pb 4f binding energof PbS nanocrystals before and after surface ligand exchange treatments. 198
Figure 9.2 Scheme of PbS nanocrystals before and after surface ligand exchange treatments.. 198
Figure 9.3 SEM images of perovskite material contained of (a) without PbS/I- (b) 0.5 wt% PbS/I-and (c) 1.0 wt% PbS/I-. (d) Scheme of crystal growth process of perovskite with or without PbS/I- seed. (e) XRD of perovskite films with various amount of PbS/I- nuclei. 202
Figure 9.4 (a) Current density-voltage (J-V) characteristics and (b) Incident photon-to-electron efficiencies (IPCEs) of the perovskite solar cells without and with various concentrations of PbS/I- seeds, measured under AM 1.5 illumination. 205
Figure 9.5 (a) The structure of TRPL quenching measured system. TRPL measurements taken at the peak emission wavelength of the (B) without PbS/I- and (C) 1.0 wt% PbS/I- based perovskite with an electron (PCBM; green curve) or hole (Spiro-OMeTAD; blue curve) quencher layer, along with stretched exponential fits to the without quenching layer data (black and red curves) and fits to the quenching samples by using the diffusion model. 208
 
Table Index
Table 4.1 Photovoltaic performances obtained from DSSCs with various CEs under AM 1.5 illumination at 100 mW cm-2. 77
Table 4.2 Parameters of EIS and Tafel polarization, and corresponding surface roughness of various CEs. 82
Table 5.1 Effect of introduce P(VDF-TrFE) into working electrode on the photovoltaic and EIS parameters under AM 1.5 illumination of 100 mW cm-2. 110
Table 7.1 Perovskite photovoltaic parameters reaction with various concentrations of MAI solution under AM 1.5 illumination at 100 mW cm-2, and corresponding lifetimes by fitting the TRPL decay profile. 145
Table 8.1 Detailed parameters of the photovoltaic performances of BI-typed CH3NH3PbI3/TiO2 NRs hybrid solar cells with TiO2 NRs under various ligand exchange treatments of OA, PYR and ACR. The device performances of the pristine planar CH3NH3PbI3 perovskite solar cell were also shown. 181
Table 8.2 Detailed device performance parameters of BI-typed CH3NH3PbI3/TiO2 NRs hybrid solar cells with various ACR-capped TiO2 NRs concentrations. 186
Table 9.1 Device performance parameters and diffusion lengths of PbS/I- based CH3NH3PbI3-xClx solar cells with various iodide-capped PbS concentrations. 204
dc.language.isoen
dc.subject硫化鉛zh_TW
dc.subject染料敏化太陽能電池zh_TW
dc.subject鈣鈦礦太陽能電池zh_TW
dc.subject二硫化鐵zh_TW
dc.subjectP(VDF-TrFE)zh_TW
dc.subject二氧化鈦奈米柱zh_TW
dc.subjectP(VDF-TrFE)en
dc.subjectlead sulfideen
dc.subjectTiO2 nanorodsen
dc.subjectDye-sensitized solar cellsen
dc.subjectperovskite solar cellsen
dc.subjectiron disulfideen
dc.title奈米材料於染料及鈣鈦礦敏化太陽能電池之應用zh_TW
dc.titleNanomaterials in Dye and Perovskite Sensitized Solar Cellsen
dc.typeThesis
dc.date.schoolyear103-2
dc.description.degree博士
dc.contributor.oralexamcommittee溫政彥,陳良益,邱雅萍,鄭有舜,余慈顏
dc.subject.keyword染料敏化太陽能電池,鈣鈦礦太陽能電池,二硫化鐵,P(VDF-TrFE),二氧化鈦奈米柱,硫化鉛,zh_TW
dc.subject.keywordDye-sensitized solar cells,perovskite solar cells,iron disulfide,P(VDF-TrFE),TiO2 nanorods,lead sulfide,en
dc.relation.page219
dc.rights.note有償授權
dc.date.accepted2015-08-19
dc.contributor.author-college工學院zh_TW
dc.contributor.author-dept材料科學與工程學研究所zh_TW
顯示於系所單位:材料科學與工程學系

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