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1

Assi, Ahmed Ali, Wasan R. Saleh, and Ezzedin Mohajerani. "Effect of Deposit Au thin Layer Between Layers of Perovskite Solar Cell on Cell's Performance." Iraqi Journal of Physics (IJP) 19, no. 51 (2021): 23–32. http://dx.doi.org/10.30723/ijp.v19i51.696.

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The present work aims to fabricate n-i-p forward perovskite solar cell (PSC) withئ structure (FTO/ compact TiO2/ compact TiO2/ MAPbI3 Perovskite/ hole transport layer/ Au). P3HT, CuI and Spiro-OMeTAD were used as hole transport layers. A nano film of 25 nm gold layer was deposited once between the electron transport layer and the perovskite layer, then between the hole transport layer and the perovskite layer. The performance of the forward-perovskite solar cell was studied. Also, the role of each electron transport layer and the hole transport layer in the perovskite solar cell was presented.
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2

Vasan, R., H. Salman, and M. O. Manasreh. "All inorganic quantum dot light emitting devices with solution processed metal oxide transport layers." MRS Advances 1, no. 4 (2016): 305–10. http://dx.doi.org/10.1557/adv.2016.129.

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ABSTRACTAll inorganic quantum dot light emitting devices with solution processed transport layers are investigated. The device consists of an anode, a hole transport layer, a quantum dot emissive layer, an electron transport layer and a cathode. Indium tin oxide coated glass slides are used as substrates with the indium tin oxide acting as the transparent anode electrode. The transport layers are both inorganic, which are relatively insensitive to moisture and other environmental factors as compared to their organic counterparts. Nickel oxide acts as the hole transport layer, while zinc oxide
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3

Wang, Yuxin, and Sin Tee Tan. "Composition of Electron Transport Layers in Organic Solar Cells (OSCs)." Highlights in Science, Engineering and Technology 12 (August 26, 2022): 99–105. http://dx.doi.org/10.54097/hset.v12i.1411.

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The research on organic solar cells has attracted researcher attention because of their flexibility, low cost and relatively simple processing methods. However, the efficiency issue is the shortcoming of organic solar energy, and one of the key factors affecting the power conversion rate is the utilization of electron transport layer. Among the materials used for the electron transport layer, metal oxides are widely used due to their stability, ease of preparation and tunable energy band structure. This article review the advantages and disadvantages of metal oxides as electron transport layer
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4

Yusuf, Abubakar Sadiq, A. M. Ramalan, A. A. Abubakar, and I. K. Mohammed. "Progress on Electron Transport Layers for Perovskite Solar Cells." Nigerian Journal of Physics 32, no. 4 (2024): 81–90. http://dx.doi.org/10.62292/njp.v32i4.2023.156.

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The photovoltaic industry is very interested in designing and developing next-generation device architectures using organic-inorganic perovskite hybrid solar cell materials. In fact, perovskites represent one of the most promising materials for high efficiency, low-cost solar cells. This is most apparent in the power conversion efficiency of perovskite solar cells (PSCs) going from 3.8 to 24.2 % in recent years. One of the primary challenges of developing PSC’s however is the realization of an appropriate electron transport layer. As such, this review focuses on recent developments in the elec
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5

Li, Bairu, Jieming Zhen, Yangyang Wan, et al. "Steering the electron transport properties of pyridine-functionalized fullerene derivatives in inverted perovskite solar cells: the nitrogen site matters." Journal of Materials Chemistry A 8, no. 7 (2020): 3872–81. http://dx.doi.org/10.1039/c9ta12188a.

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Three pyridine-functionalized fullerene derivatives with variable nitrogen sites were synthesized and used as electron transport layers of iPSCs, exhibiting tunable interactions with the perovskite layer and different electron transport properties.
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6

Vannikov, Anatolii V., Antonina D. Grishina, and S. V. Novikov. "Electron transport and electroluminescence in polymer layers." Russian Chemical Reviews 63, no. 2 (1994): 103–23. http://dx.doi.org/10.1070/rc1994v063n02abeh000074.

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7

Synowiec, Z., and B. Paszkiewicz. "Electron transport in implant isolation GaAs layers." Microelectronics Reliability 43, no. 4 (2003): 675–79. http://dx.doi.org/10.1016/s0026-2714(03)00016-7.

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8

Moiz, Syed Abdul. "Optimization of Hole and Electron Transport Layer for Highly Efficient Lead-Free Cs2TiBr6-Based Perovskite Solar Cell." Photonics 9, no. 1 (2021): 23. http://dx.doi.org/10.3390/photonics9010023.

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The methylammonium lead halide solar cell has attracted a great deal of attention due to its lightweight, low cost, and simple fabrication and processing. Despite these advantages, these cells are still far from commercialization because of their lead-based toxicity. Among lead-free perovskites, cesium-titanium (IV) bromide (Cs2TiBr6) is considered one of the best alternatives, but it faces a lack of higher PCE (power conversion efficiency) due to the unavailability of the matched hole and electron transport layers. Therefore, in this study, the ideal hole and electron transport layer paramete
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9

Rani, R., K. Monga, and S. Chaudhary. "Recent development in electron transport layers for efficient tin-based perovskite solar cells." IOP Conference Series: Materials Science and Engineering 1258, no. 1 (2022): 012015. http://dx.doi.org/10.1088/1757-899x/1258/1/012015.

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Hybrid organic-inorganic tin (Sn)-based perovskite materials became a promising choice as an alternative to lead-free perovskite solar cells (PSCs) due to their outstanding optical and electrical properties. But, so far, a power conversion efficiency (PCE) of only 13% has been achieved for Sn-based PSCs. To achieve highly efficient and stable PSCs, not only the properties of the active layer but the charge selective contacts (electron and hole transport layers) should be selected wisely. The interfaces between the perovskite active layer and charge transport layers play an important role in ac
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10

Mityashin, Alexander, David Cheyns, Barry P. Rand, and Paul Heremans. "Understanding metal doping for organic electron transport layers." Applied Physics Letters 100, no. 5 (2012): 053305. http://dx.doi.org/10.1063/1.3681383.

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11

Bailey, G. R. "Two-dimensional electron transport in InP surface layers." Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures 5, no. 4 (1987): 976. http://dx.doi.org/10.1116/1.583828.

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12

Wei, Huiyun, Jionghua Wu, Peng Qiu, et al. "Plasma-enhanced atomic-layer-deposited gallium nitride as an electron transport layer for planar perovskite solar cells." Journal of Materials Chemistry A 7, no. 44 (2019): 25347–54. http://dx.doi.org/10.1039/c9ta08929b.

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13

Kim, Yujin, Sung Hwan Joo, Seong Gwan Shin, et al. "Effect of Annealing in ITO Film Prepared at Various Argon-and-Oxygen-Mixture Ratios via Facing-Target Sputtering for Transparent Electrode of Perovskite Solar Cells." Coatings 12, no. 2 (2022): 203. http://dx.doi.org/10.3390/coatings12020203.

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Normal perovskite solar cells (PSCs) consist of the following layers: transparent electrode, electron-transport layer (ETL), light-absorbing perovskite layer, hole-transport layer (HTL), and metal electrode. Energy, such as electricity, is produced through light absorbance and electron–hole generation/transport between two electrode types (metal film and transparent conducting film). Among stacked layers in a PSC, the transparent electrode plays the high-performance-power-conversion-efficiency role. Transparent electrodes should have high-visible-range transparency and low resistance. Therefor
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14

Yang, Jien, Qiong Zhang, Jinjin Xu, et al. "All-Inorganic Perovskite Solar Cells Based on CsPbIBr2 and Metal Oxide Transport Layers with Improved Stability." Nanomaterials 9, no. 12 (2019): 1666. http://dx.doi.org/10.3390/nano9121666.

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Despite the successful improvement in the power conversion efficiency (PCE) of perovskite solar cells (PSCs), the issue of instability is still a serious challenge for their commercial application. The issue of the PSCs mainly originates from the decomposition of the organic–inorganic hybrid perovskite materials, which will degrade upon humidity and suffer from the thermal environment. In addition, the charge transport layers also influence the stability of the whole devices. In this study, inorganic transport layers are utilized in an inverted structure of PSCs employing CsPbIBr2 as light abs
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15

Jang, Ji Geun, and Hyun Jin Ji. "Blue Phosphorescent Organic Light-Emitting Devices with the Emissive Layer of mCP:FCNIr(pic)." Advances in Materials Science and Engineering 2012 (2012): 1–5. http://dx.doi.org/10.1155/2012/192731.

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New high-efficiency blue-light-emitting phosphorescent devices with 300 Å-thick emissive layer of N,N′-dicarbazolyl-3,5-benzene [mCP] doped with 10 vol.% bis[(3,5-difluoro-4-cyanophenyl)pyridine]iridium picolinate [FCNIr(pic)] were fabricated with the different treatments of hole and electron transport layers. In the experiments, a single layer of 1,1-bis-(di-4-polyaminophenyl)cyclohexane [TAPC] and a double layer of N,N′-di(1-naphthyl)-N,N′-diphenylbenzidine [NPB] and mCP were used as hole transport layers (HTLs). In addition, 500 Å-thick double layers of tris-[3-(3-pyridyl)mesityl]borane [3T
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16

Rashed, Shukri, Vishnu Vilas Kutwade, Ketan Prakash Gattu, Ghamdan Mahmood Mohammed Saleh Gubari, and Ramphal Sharma. "Growth and Exploration of Inorganic Semiconductor Electron and Hole Transport Layers for Low-Cost Perovskite Solar Cells." Trends in Sciences 20, no. 10 (2023): 5839. http://dx.doi.org/10.48048/tis.2023.5839.

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The perovskite exhibited outstanding performance and was a promising alternative material for a low-cost, high power conversion efficiency (PCE) solar cell application. To avoid the high-cost organic materials as electron transport layers (ETL) and hole transport layers (HTL) in perovskite solar cells (PSCs), here introduce the inorganic semiconductor nanomaterials ZnS and CuS work as an ETL and HTL, respectively. In this work, we selected chalcogenides such as zinc sulfide (ZnS) and copper sulfide (CuS) as the 2-electron and hole transport layers and utilized them for perovskite solar cell ap
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17

Davis, Denet, M. S. Shamna, K. S. Nithya, and K. S. Sudheer. "Graphene as a hole transport layer for enhanced performance of P3HT: PCBM bulk heterojunction organic solar cell: a numerical simulation study." IOP Conference Series: Materials Science and Engineering 1248, no. 1 (2022): 012011. http://dx.doi.org/10.1088/1757-899x/1248/1/012011.

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Abstract As sustainable and green energy technologies advance, academic and industrial researchers have been more interested in organic solar cells. Organic solar cells have some key advantages, such as lightweight, flexibility and cheapness that make them an ideal choice as an alternative to other types of solar cells. Bulk heterojunction solar cells combine the advantages of easier fabrication and higher conversion efficiency, making them the best structure currently. In this work P3HT: PCBM is used as the active layer material. PDINO and PFN-Br are used as the electron transport layers in t
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18

Mizuta, Yosuke, Mayumi Nagayama, Kazunari Sasaki, and Akari Hayashi. "Investigation of a Method of Evaluating Proton Transport Resistance in PEFC Catalyst Layers." ECS Transactions 109, no. 9 (2022): 369–77. http://dx.doi.org/10.1149/10909.0369ecst.

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Since there is no method to directly measure proton conductivity in the catalyst layer in PEFC even though proton conduction in the catalyst layer is one of the critical factors for high performance and durability. A method to directly measure proton transport resistance in the catalyst layers was investigated by sandwiching a sample layer by two Nafion® membranes to block electron transfer, and two gas diffusion electrodes to reduce gas diffusion resistance, in this study. Direct current was applied to the system in the hydrogen atmosphere, and measurements for proton transport resistance wer
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19

McCarthy, Melissa M., Arnaud Walter, Soo-Jin Moon, et al. "Atomic Layer Deposited Electron Transport Layers in Efficient Organometallic Halide Perovskite Devices." MRS Advances 3, no. 51 (2018): 3075–84. http://dx.doi.org/10.1557/adv.2018.515.

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ABSTRACTAmorphous TiO2 and SnO2 electron transport layers (ETLs) were deposited by low-temperature atomic layer deposition (ALD). Surface morphology and x-ray photoelectron spectroscopy (XPS) indicate uniform and pinhole free coverage of these ALD hole blocking layers. Both mesoporous and planar perovskite solar cells were fabricated based on these thin films with aperture areas of 1.04 cm2 for TiO2 and 0.09 cm2 and 0.70 cm2 for SnO2. The resulting cell performance of 18.3 % power conversion efficiency (PCE) using planar SnO2 on 0.09 cm2 and 15.3 % PCE using mesoporous TiO2 on 1.04 cm2 active
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20

Mehdi, S., R. Amraoui, and A. Aissat. "Numerical investigation of organic light emitting diode OLED with different hole transport materials." Digest Journal of Nanomaterials and Biostructures 17, no. 3 (2022): 781. http://dx.doi.org/10.15251/djnb.2022.173.781.

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In this paper, a comparative study between four OLEDs devices is carried out. The bi- layers device (A) (consists of) Hole Injection Layer (HIL)/Electron Transport Layer (ETL), the multilayer device (B) (consists of) HIL Layer/Hole Transport Layer (HTL)/ETL Layer. The influence of the hole transporting material on the performance of the three layers OLEDs was investigated. Three different HTL materials were used: α- NPD, TAPC and p-TTA with the same electron transporting material as Alq3; (these holes transport material consists the devices (B), (C) and (D) respectively). The carrier injection
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21

Friedl, Jared D., Ramez Hosseinian Ahangharnejhad, Adam B. Phillips, and Michael J. Heben. "Materials requirements for improving the electron transport layer/perovskite interface of perovskite solar cells determined via numerical modeling." MRS Advances 5, no. 50 (2020): 2603–10. http://dx.doi.org/10.1557/adv.2020.319.

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AbstractPerovskite solar cells continue to garner significant attention in the field of photovoltaics. As the optoelectronic properties of the absorbers become better understood, attention has turned to more deeply understanding the contribution of charge transport layers for efficient extraction of carriers. Titanium oxide is known to be an effective electron transport layer (ETL) in planar perovskite solar cells, but it is unlikely to result in the best device performance possible. To investigate the importance of band energy alignment between the electron transport layer and perovskite, we
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22

Jung, Jaroslaw, Arkadiusz Selerowicz, Paulina Maczugowska, et al. "Electron Transport in Naphthalene Diimide Derivatives." Materials 14, no. 14 (2021): 4026. http://dx.doi.org/10.3390/ma14144026.

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Two naphthalene diimides derivatives containing two different (alkyl and alkoxyphenyl) N-substituents were studied, namely, N,N′-bis(sec-butyl)-1,4,5,8-naphthalenetetracarboxylic acid diimide (NDI-s-Bu) and N,N′-bis(4-n-hexyloxyphenyl)-1,4,5,8-naphthalenetetracarboxylic acid diimide (NDI-4-n-OHePh). These compounds are known to exhibit electron transport due to their electron-deficient character evidenced by high electron affinity (EA) values, determined by electrochemical methods and a low-lying lowest unoccupied molecular orbital (LUMO) level, predicted by density functional theory (DFT) cal
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23

Shih, Wei-Kai, Srinivas Jallepalli, Mahbub Rashed, Christine M. Maziar, and Al F. Tasch Jr. "Study of Electron Velocity Overshoot in NMOS Inversion Layers." VLSI Design 8, no. 1-4 (1998): 429–35. http://dx.doi.org/10.1155/1998/65364.

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Non-local electron transport in nMOSFET inversion layers has been studied by Monte Carlo (MC) simulations. Inversion layer quantization has been explicitly included in the calculation of density of states and scattering rate for low-energy electrons while bulk band structure is used to describe the transport of more energetic electrons. For uniform, high-lateral field conditions, the effects of quantization are less pronounced due to the depopulation of electrons in the lower-lying subbands. On the other hand, Monte Carlo results for carrier transport in spatially varying lateral fields (such
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24

Kwak, Hee Jung, Collins Kiguye, Minsik Gong, Jun Hong Park, Gi-Hwan Kim, and Jun Young Kim. "Enhanced Performance of Inverted Perovskite Quantum Dot Light-Emitting Diode Using Electron Suppression Layer and Surface Morphology Control." Materials 16, no. 22 (2023): 7171. http://dx.doi.org/10.3390/ma16227171.

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The energy level offset at inorganic layer–organic layer interfaces and the mismatch of hole/electron mobilities of the individual layers greatly limit the establishment of balanced charge carrier injection inside the emissive layer of halide perovskite light-emitting diodes (PeQLEDs). In contrast with other types of light-emitting devices, namely OLEDs and QLEDs, various techniques such as inserting an electron suppression layer between the emissive and electron transport layer have been employed as a means of establishing charge carrier injection into their respective emissive layers. Hence,
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25

Jana, Atanu, Vijaya Gopalan Sree, Qiankai Ba, et al. "Efficient organic manganese(ii) bromide green-light-emitting diodes enabled by manipulating the hole and electron transport layer." Journal of Materials Chemistry C 9, no. 34 (2021): 11314–23. http://dx.doi.org/10.1039/d1tc02550c.

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26

Curzon, A. E. "The structure and properties of misfit layer compounds." Proceedings, annual meeting, Electron Microscopy Society of America 54 (August 11, 1996): 708–9. http://dx.doi.org/10.1017/s0424820100166002.

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The purpose of this article is to provide an introduction to the class of compounds known as misfit layer compounds.An example of a misfit layer compound is (NdS)1.2NbS2 In the present study this material was made by heating appropriate amounts of sulphur powder, niobium powder and neodymium chips in an evacuated quartz tube at 850°C for 12 hours. A subsequent five day process involving transport and back transport at 1000°C in the presence of iodine as transport agent led to the formation of lustrous crystal platelets suitable for electron microscopy and electron diffraction studies. The orth
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Li, Chang, Ge Wang, Yajun Gao, et al. "Highly efficient polymer solar cells based on low-temperature processed ZnO: application of a bifunctional Au@CNTs nanocomposite." Journal of Materials Chemistry C 7, no. 9 (2019): 2676–85. http://dx.doi.org/10.1039/c8tc05653f.

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28

Erdogar, Kubra, Ozgun Yucel, and Muhammed Enes Oruc. "Investigation of Structural, Morphological, and Optical Properties of Novel Electrospun Mg-Doped TiO2 Nanofibers as an Electron Transport Material for Perovskite Solar Cells." Nanomaterials 13, no. 15 (2023): 2255. http://dx.doi.org/10.3390/nano13152255.

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Perovskite solar cells (PSCs) are quickly becoming efficient solar cells due to the effective physicochemical properties of the absorber layer. This layer should ideally be placed between a stable hole transport material (HTM) layer and a conductive electron transport material (ETM) layer. These outer layers play a critical role in the current densities and cell voltages of solar cells. In this work, we successfully fabricated Mg-doped TiO2 nanofibers as ETM layers via electrospinning. This study systematically investigates the morphological and optical features of Mg-doped nanofibers as mesop
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Jenkins, Michael B., Barbara S. Eaglesham, Larry C. Anthony, Scott C. Kachlany, Dwight D. Bowman, and William C. Ghiorse. "Significance of Wall Structure, Macromolecular Composition, and Surface Polymers to the Survival and Transport of Cryptosporidium parvum Oocysts." Applied and Environmental Microbiology 76, no. 6 (2010): 1926–34. http://dx.doi.org/10.1128/aem.02295-09.

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ABSTRACT The structure and composition of the oocyst wall are primary factors determining the survival and hydrologic transport of Cryptosporidium parvum oocysts outside the host. Microscopic and biochemical analyses of whole oocysts and purified oocyst walls were undertaken to better understand the inactivation kinetics and hydrologic transport of oocysts in terrestrial and aquatic environments. Results of microscopy showed an outer electron-dense layer, a translucent middle layer, two inner electron-dense layers, and a suture structure embedded in the inner electron-dense layers. Freeze-subs
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Vogelsang, Th, and K. R. Hofmann. "Electron transport in strained Si layers on Si1−xGexsubstrates." Applied Physics Letters 63, no. 2 (1993): 186–88. http://dx.doi.org/10.1063/1.110394.

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31

Osman, M. A. "Minority electron transport acrossp+doped submicron layers of GaAs." Journal of Applied Physics 71, no. 1 (1992): 308–13. http://dx.doi.org/10.1063/1.350707.

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Roldán, J. B., F. Gámiz, J. A. López Villanueva, and P. Caetujo. "Electron transport properties of quantized silicon carbide inversion layers." Journal of Electronic Materials 26, no. 3 (1997): 203–7. http://dx.doi.org/10.1007/s11664-997-0151-3.

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Patil, M. B., Y. Okuyama, Y. Ohkura, T. Toyabe, and S. Ihara. "Transmission matrix approach for electron transport in inversion layers." Solid-State Electronics 37, no. 7 (1994): 1359–65. http://dx.doi.org/10.1016/0038-1101(94)90192-9.

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Thakur, Ujwal, Ryan Kisslinger, and Karthik Shankar. "One-Dimensional Electron Transport Layers for Perovskite Solar Cells." Nanomaterials 7, no. 5 (2017): 95. http://dx.doi.org/10.3390/nano7050095.

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CHEN Ya-wen, 陈亚文, 黄. 航. HUANG Hang, 魏雄伟 WEI Xiong-wei, et al. "QLEDs with Organic/Inorganic Hybrid Double Electron Transport Layers." Chinese Journal of Luminescence 39, no. 10 (2018): 1439–44. http://dx.doi.org/10.3788/fgxb20183910.1439.

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Kojima, H., M. E. Gershenson, V. M. Pudalov, G. Brunthaler, A. Prinz, and G. Bauer. "Interaction Effects in Electron Transport in Si Inversion Layers." Journal of the Physical Society of Japan 72, Suppl.A (2003): 57–62. http://dx.doi.org/10.1143/jpsjs.72sa.57.

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Chetverikov, A. P., W. Ebeling, G. Röpke, and M. G. Velarde. "Electron Transport Mediated by Nonlinear Excitations in Atomic Layers." Contributions to Plasma Physics 53, no. 4-5 (2013): 355–59. http://dx.doi.org/10.1002/ctpp.201200124.

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38

Choi, Jongmin, Jea Woong Jo, F. Pelayo García de Arquer, et al. "Activated Electron-Transport Layers for Infrared Quantum Dot Optoelectronics." Advanced Materials 30, no. 29 (2018): 1801720. http://dx.doi.org/10.1002/adma.201801720.

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39

Son, Hyojung, and Byoung-Seong Jeong. "Optimization of the Power Conversion Efficiency of CsPbIxBr3−x-Based Perovskite Photovoltaic Solar Cells Using ZnO and NiOx as an Inorganic Charge Transport Layer." Applied Sciences 12, no. 18 (2022): 8987. http://dx.doi.org/10.3390/app12188987.

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In this study, we analyzed the maximum power conversion efficiency (PCE) of a photovoltaic cell with an ITO/ZnO/CsPbIxBr3−x/NiOx/Au structure, using ZnO and NiOx as the inorganic charge transport layers and CsPbIxBr3−x as an absorption layer. We optimized the thickness of each layer and investigated the effects of the defect density and interface defect density. To achieve the highest PCE, the optimal thicknesses were 300 nm for the electron transport layer (ZnO), 60 nm for the hole transport layer (NiOx), and 1000 nm for the absorption layer. The absorber defect density was maintained at appr
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Nguyen, Nguyen, Nguyen, et al. "Recent Progress in Carbon-Based Buffer Layers for Polymer Solar Cells." Polymers 11, no. 11 (2019): 1858. http://dx.doi.org/10.3390/polym11111858.

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Carbon-based materials are promising candidates as charge transport layers in various optoelectronic devices and have been applied to enhance the performance and stability of such devices. In this paper, we provide an overview of the most contemporary strategies that use carbon-based materials including graphene, graphene oxide, carbon nanotubes, carbon quantum dots, and graphitic carbon nitride as buffer layers in polymer solar cells (PSCs). The crucial parameters that regulate the performance of carbon-based buffer layers are highlighted and discussed in detail. Furthermore, the performances
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Tarique, Walia Binte, Md Habibur Rahaman, Shahriyar Safat Dipta, Ashraful Hossain Howlader, and Ashraf Uddin. "Solution-Processed Bilayered ZnO Electron Transport Layer for Efficient Inverted Non-Fullerene Organic Solar Cells." Nanomanufacturing 4, no. 2 (2024): 81–98. http://dx.doi.org/10.3390/nanomanufacturing4020006.

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Organic solar cells (OSCs) are becoming increasingly popular in the scientific community because of their many desirable properties. These features include solution processability, low weight, low cost, and the ability to process on a wide scale using roll-to-roll technology. Enhancing the efficiency of photovoltaic systems, particularly high-performance OSCs, requires study into not only material design but also interface engineering. This study demonstrated that two different types of OSCs based on the PTB7-Th:IEICO-4F and PM6:Y6 active layers use a ZnO bilayer electron transport layer (ETL)
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Cui Yupeng, 崔玉鹏, 弓爵 Gong Jue та 刘明侦 Liu Mingzhen. "钙钛矿太阳能电池中的二氧化锡电子传输层调控". Laser & Optoelectronics Progress 61, № 5 (2024): 0516002. http://dx.doi.org/10.3788/lop230905.

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Huang, Wen, Rui Zhang, Xuwen Xia, et al. "Room Temperature Processed Double Electron Transport Layers for Efficient Perovskite Solar Cells." Nanomaterials 11, no. 2 (2021): 329. http://dx.doi.org/10.3390/nano11020329.

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Zinc Oxide (ZnO) has been regarded as a promising electron transport layer (ETL) in perovskite solar cells (PSCs) owing to its high electron mobility. However, the acid-nonresistance of ZnO could destroy organic-inorganic hybrid halide perovskite such as methylammonium lead triiodide (MAPbI3) in PSCs, resulting in poor power conversion efficiency (PCE). It is demonstrated in this work that Nb2O5/ZnO films were deposited at room temperature with RF magnetron sputtering and were successfully used as double electron transport layers (DETL) in PSCs due to the energy band matching between Nb2O5 and
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44

Ivanova, A., A. Tokmakov, K. Lebedeva, M. Roze, and I. Kaulachs. "Influence of the Preparation Method on Planar Perovskite CH3NH3PbI3-xClx Solar Cell Performance and Hysteresis." Latvian Journal of Physics and Technical Sciences 54, no. 4 (2017): 58–68. http://dx.doi.org/10.1515/lpts-2017-0027.

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Abstract Organometal halide perovskites are promising materials for lowcost, high-efficiency solar cells. The method of perovskite layer deposition and the interfacial layers play an important role in determining the efficiency of perovskite solar cells (PSCs). In the paper, we demonstrate inverted planar perovskite solar cells where perovskite layers are deposited by two-step modified interdiffusion and one-step methods. We also demonstrate how PSC parameters change by doping of charge transport layers (CTL). We used dimethylsupoxide (DMSO) as dopant for the hole transport layer (PEDOT:PSS) b
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Chang, Tsung-Wen, Chzu-Chiang Tseng, Dave W. Chen, Gwomei Wu, Chia-Ling Yang, and Lung-Chien Chen. "Preparation and Characterization of Thin-Film Solar Cells with Ag/C60/MAPbI3/CZTSe/Mo/FTO Multilayered Structures." Molecules 26, no. 12 (2021): 3516. http://dx.doi.org/10.3390/molecules26123516.

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New solar cells with Ag/C60/MAPbI3/Cu2ZnSnSe4 (CZTSe)/Mo/FTO multilayered structures on glass substrates have been prepared and investigated in this study. The electron-transport layer, active photovoltaic layer, and hole-transport layer were made of C60, CH3NH3PbI3 (MAPbI3) perovskite, and CZTSe, respectively. The CZTSe hole-transport layers were deposited by magnetic sputtering, with the various thermal annealing temperatures at 300 °C, 400 °C, and 500 °C, and the film thickness was also varied at 50~300 nm The active photovoltaic MAPbI3 films were prepared using a two-step spin-coating meth
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Deo, Meenal, Alexander Möllmann, Jinane Haddad, et al. "Tantalum Oxide as an Efficient Alternative Electron Transporting Layer for Perovskite Solar Cells." Nanomaterials 12, no. 5 (2022): 780. http://dx.doi.org/10.3390/nano12050780.

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Electron transporting layers facilitating electron extraction and suppressing hole recombination at the cathode are crucial components in any thin-film solar cell geometry, including that of metal–halide perovskite solar cells. Amorphous tantalum oxide (Ta2O5) deposited by spin coating was explored as an electron transport material for perovskite solar cells, achieving power conversion efficiency (PCE) up to ~14%. Ultraviolet photoelectron spectroscopy (UPS) measurements revealed that the extraction of photogenerated electrons is facilitated due to proper alignment of bandgap energies. Steady-
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Yusuf, Abubakar S., A. M. Ramalan, A. A. Abubakar, and I. K. Mohammed. "Effect of Electron Transport Layers, Interface Defect Density and Working Temperature on Perovskite Solar Cells Using SCAPS 1-D Software." East European Journal of Physics, no. 1 (March 5, 2024): 332–41. http://dx.doi.org/10.26565/2312-4334-2024-1-31.

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Perovskite solar cells have garnered significant attention from solar cell researchers due to their potential for achieving high efficiency, primarily attributed to their exceptional Electron Transport layer (ETL). One of the key elements of perovskite solar cells for transporting electrons to generate current is the ETL material. Moreover, there is a promising avenue for enhancing stability and reducing fabrication costs by substituting the transport layer. In this study, TiO2 and SnO2 were used as ETL materials in the architecture of perovskite solar cells for a comparative analysis between
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Hattori, Nagisa, Kazuhiro Manseki, Yuto Hibi, et al. "Simultaneous Li-Doping and Formation of SnO2-Based Composites with TiO2: Applications for Perovskite Solar Cells." Materials 17, no. 10 (2024): 2339. http://dx.doi.org/10.3390/ma17102339.

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Tin oxide (SnO2) has been recognized as one of the beneficial components in the electron transport layer (ETL) of lead–halide perovskite solar cells (PSCs) due to its high electron mobility. The SnO2-based thin film serves for electron extraction and transport in the device, induced by light absorption at the perovskite layer. The focus of this paper is on the heat treatment of a nanoaggregate layer of single-nanometer-scale SnO2 particles in combination with another metal-dopant precursor to develop a new process for ETL in PSCs. The combined precursor solution of Li chloride and titanium(IV)
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Rani, Sweta, and Jitendra Kumar. "Modeling charge transport mechanism in inorganic quantum dot light-emitting devices through transport layer modification strategies." Journal of Applied Physics 133, no. 10 (2023): 104302. http://dx.doi.org/10.1063/5.0139599.

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Quantum dot light-emitting devices (QLEDs) are potential candidates for lighting and display applications. The charge transport mechanism which plays an essential part in the performance of these devices, however, needs to be explored and analyzed for further improvement. The imbalance of the injection and transport of charge carriers within the device adversely affects the efficiency and stability of the device. Charge balance can be improved by better charge injection of holes while suppressing the excessive electrons. A simple and effective strategy to achieve this is using double transport
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Pham, Hoang Minh, Syed Dildar Haider Naqvi, Huyen Tran, et al. "Effects of the Electrical Properties of SnO2 and C60 on the Carrier Transport Characteristics of p-i-n-Structured Semitransparent Perovskite Solar Cells." Nanomaterials 13, no. 24 (2023): 3091. http://dx.doi.org/10.3390/nano13243091.

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Recently, metal halide perovskite-based top cells have shown significant potential for use in inexpensive and high-performance tandem solar cells. In state-of-the-art p-i-n perovskite/Si tandem devices, atomic-layer-deposited SnO2 has been widely used as a buffer layer in the top cells because it enables conformal, pinhole-free, and highly transparent buffer layer formation. In this work, the effects of various electrical properties of SnO2 and C60 layers on the carrier transport characteristics and the performance of the final devices were investigated using a numerical simulation method, whi
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