- Sort by:
- Newest first
- Titles A to Z
Filter by subject:
- Physics [95]
- Cross-disciplinary physics and related areas of science and technology [95]
- Energy research and environmental science [95]
- Energy conversion [95]
- Photoelectric conversion; solar cells and arrays [95]
- Electrical and electronic engineering [95]
- Components, electron devices and materials [95]
- Power systems and applications [93]
- Direct energy conversion and energy storage [93]
- Solar cells and arrays [93]
- [89]
- http://iet.metastore.ingenta.com/content/subject/b2550,http://iet.metastore.ingenta.com/content/subject/a8100,http://iet.metastore.ingenta.com/content/subject/a7000,http://iet.metastore.ingenta.com/content/subject/b2520,http://iet.metastore.ingenta.com/content/subject/b0000,http://iet.metastore.ingenta.com/content/subject/b2560,http://iet.metastore.ingenta.com/content/subject/a6000,http://iet.metastore.ingenta.com/content/subject/b0500,http://iet.metastore.ingenta.com/content/subject/b2530,http://iet.metastore.ingenta.com/content/subject/a7300,http://iet.metastore.ingenta.com/content/subject/a8115,http://iet.metastore.ingenta.com/content/subject/b0520,http://iet.metastore.ingenta.com/content/subject/b2550e,http://iet.metastore.ingenta.com/content/subject/a6800,http://iet.metastore.ingenta.com/content/subject/a8160,http://iet.metastore.ingenta.com/content/subject/b2520c,http://iet.metastore.ingenta.com/content/subject/b2560b,http://iet.metastore.ingenta.com/content/subject/a7200,http://iet.metastore.ingenta.com/content/subject/a7340,http://iet.metastore.ingenta.com/content/subject/a8160c,http://iet.metastore.ingenta.com/content/subject/a6100,http://iet.metastore.ingenta.com/content/subject/a8115h,http://iet.metastore.ingenta.com/content/subject/b0520f,http://iet.metastore.ingenta.com/content/subject/a6855,http://iet.metastore.ingenta.com/content/subject/b4000,http://iet.metastore.ingenta.com/content/subject/b2530f,http://iet.metastore.ingenta.com/content/subject/a6170,http://iet.metastore.ingenta.com/content/subject/a7340q,http://iet.metastore.ingenta.com/content/subject/e,http://iet.metastore.ingenta.com/content/subject/e1000,http://iet.metastore.ingenta.com/content/subject/e1500,http://iet.metastore.ingenta.com/content/subject/e1520,http://iet.metastore.ingenta.com/content/subject/e1520n,http://iet.metastore.ingenta.com/content/subject/e3000,http://iet.metastore.ingenta.com/content/subject/e3600,http://iet.metastore.ingenta.com/content/subject/e3644,http://iet.metastore.ingenta.com/content/subject/e3644a,http://iet.metastore.ingenta.com/content/subject/a4000,http://iet.metastore.ingenta.com/content/subject/a5000,http://iet.metastore.ingenta.com/content/subject/a5200,http://iet.metastore.ingenta.com/content/subject/a7220,http://iet.metastore.ingenta.com/content/subject/a7220j,http://iet.metastore.ingenta.com/content/subject/b2520d,http://iet.metastore.ingenta.com/content/subject/b2550b,http://iet.metastore.ingenta.com/content/subject/b2550n,http://iet.metastore.ingenta.com/content/subject/b2560h,http://iet.metastore.ingenta.com/content/subject/a6170t,http://iet.metastore.ingenta.com/content/subject/a7240,http://iet.metastore.ingenta.com/content/subject/a7360,http://iet.metastore.ingenta.com/content/subject/b2530b,http://iet.metastore.ingenta.com/content/subject/b4200,http://iet.metastore.ingenta.com/content/subject/e3644n,http://iet.metastore.ingenta.com/content/subject/a4200,http://iet.metastore.ingenta.com/content/subject/a5275,http://iet.metastore.ingenta.com/content/subject/a5275r,http://iet.metastore.ingenta.com/content/subject/a7330,http://iet.metastore.ingenta.com/content/subject/a8140,http://iet.metastore.ingenta.com/content/subject/b2200,http://iet.metastore.ingenta.com/content/subject/a0000,http://iet.metastore.ingenta.com/content/subject/a6146,http://iet.metastore.ingenta.com/content/subject/a7340l,http://iet.metastore.ingenta.com/content/subject/a7800,http://iet.metastore.ingenta.com/content/subject/a7865,http://iet.metastore.ingenta.com/content/subject/a8115g,http://iet.metastore.ingenta.com/content/subject/a8140g,http://iet.metastore.ingenta.com/content/subject/b0520d,http://iet.metastore.ingenta.com/content/subject/b2520f,http://iet.metastore.ingenta.com/content/subject/b2520m,http://iet.metastore.ingenta.com/content/subject/b2530d,http://iet.metastore.ingenta.com/content/subject/b4250,http://iet.metastore.ingenta.com/content/subject/a0100,http://iet.metastore.ingenta.com/content/subject/a4280,http://iet.metastore.ingenta.com/content/subject/a7360j,http://iet.metastore.ingenta.com/content/subject/a8116,http://iet.metastore.ingenta.com/content/subject/a8610,http://iet.metastore.ingenta.com/content/subject/a8610k,http://iet.metastore.ingenta.com/content/subject/b0100,http://iet.metastore.ingenta.com/content/subject/b0510,http://iet.metastore.ingenta.com/content/subject/b2530c,http://iet.metastore.ingenta.com/content/subject/b2550a,http://iet.metastore.ingenta.com/content/subject/b2560s,http://iet.metastore.ingenta.com/content/subject/b4100,http://iet.metastore.ingenta.com/content/subject/b8100,http://iet.metastore.ingenta.com/content/subject/b8110,http://iet.metastore.ingenta.com/content/subject/b8200,http://iet.metastore.ingenta.com/content/subject/e0000,http://iet.metastore.ingenta.com/content/subject/a0130,http://iet.metastore.ingenta.com/content/subject/a4700,http://iet.metastore.ingenta.com/content/subject/a4765
- b2550,a8100,a7000,b2520,b0000,b2560,a6000,b0500,b2530,a7300,a8115,b0520,b2550e,a6800,a8160,b2520c,b2560b,a7200,a7340,a8160c,a6100,a8115h,b0520f,a6855,b4000,b2530f,a6170,a7340q,e,e1000,e1500,e1520,e1520n,e3000,e3600,e3644,e3644a,a4000,a5000,a5200,a7220,a7220j,b2520d,b2550b,b2550n,b2560h,a6170t,a7240,a7360,b2530b,b4200,e3644n,a4200,a5275,a5275r,a7330,a8140,b2200,a0000,a6146,a7340l,a7800,a7865,a8115g,a8140g,b0520d,b2520f,b2520m,b2530d,b4250,a0100,a4280,a7360j,a8116,a8610,a8610k,b0100,b0510,b2530c,b2550a,b2560s,b4100,b8100,b8110,b8200,e0000,a0130,a4700,a4765
- [36],[34],[32],[29],[26],[25],[24],[24],[22],[20],[19],[19],[17],[16],[15],[15],[15],[14],[14],[14],[13],[13],[13],[12],[10],[9],[8],[8],[8],[8],[8],[8],[8],[8],[8],[8],[8],[7],[7],[7],[7],[7],[7],[7],[7],[7],[6],[6],[6],[6],[6],[6],[5],[5],[5],[5],[5],[5],[4],[4],[4],[4],[4],[4],[4],[4],[4],[4],[4],[4],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[3],[2],[2],[2]
- /search/morefacet;jsessionid=10ayipv9bjy3t.x-iet-live-01
- /content/searchconcept;jsessionid=10ayipv9bjy3t.x-iet-live-01?operator4=AND&pageSize=50&sortDescending=true&facetNames=pub_concept_facet+pub_concept_facet+pub_concept_facet+pub_concept_facet&value3=b&value4=b2000&value1=a8630j&value2=a&facetOptions=2+3+4+5&option1=pub_concept&option2=pub_concept_facet&option3=pub_concept_facet&option4=pub_concept_facet&sortField=prism_publicationDate&operator3=AND&operator2=AND&operator5=AND&option5=pub_concept_facet&value5=
- See more See less
Filter by content type:
Filter by publication date:
- 2018 [20]
- 1980 [8]
- 2003 [7]
- 2013 [5]
- 1984 [4]
- 1985 [4]
- 1981 [3]
- 2009 [3]
- 2017 [3]
- 1963 [2]
- 1979 [2]
- 1982 [2]
- 1983 [2]
- 2011 [2]
- 2014 [2]
- 2019 [2]
- 1976 [1]
- 1987 [1]
- 1991 [1]
- 1992 [1]
- 1993 [1]
- 1998 [1]
- 2000 [1]
- 2004 [1]
- 2005 [1]
- 2006 [1]
- 2007 [1]
- 2010 [1]
- 2015 [1]
- 2016 [1]
- See more See less
Filter by author:
- L. Castañer [3]
- O.M. Nielsen [3]
- Federica Cappelluti [2]
- G.G. Roberts [2]
- H.C. Card [2]
- J. Poortmans [2]
- L. Prat [2]
- M. Günes [2]
- M. Jeon [2]
- M.C. Petty [2]
- Mariangela Gioannini [2]
- Y.W. Lam [2]
- A. Alias [1]
- A. Criado [1]
- A. De Maria [1]
- A. Heya [1]
- A. Luque [1]
- A. Madan [1]
- A. Solanki [1]
- A. Vishnoi [1]
- A.B. Abd Rahman [1]
- A.B. Kazantsev [1]
- A.E. Zhukov [1]
- A.I.A. Rani [1]
- A.M. Nadtochiy [1]
- A.R. Es-Slassi [1]
- A.W. Bett [1]
- Abhigyan Ganguly [1]
- Ahmad Al-Mulla [1]
- Ahmad Al-Otaibi [1]
- Ali Hajjiah [1]
- Arastoo Khalili [1]
- Ariel P. Cedola [1]
- Armin G. Aberle [1]
- Armin Gerhard Aberle [1]
- Arthur Weeber [1]
- Ayman Al-Qattan [1]
- B. Alonso [1]
- B. Damilano [1]
- B. Royall [1]
- B.-P. Zhang [1]
- B.D. Choi [1]
- B.K. Ghosh [1]
- C. Agert [1]
- C. Boehme [1]
- C. Carvalho [1]
- C. Ornaghi [1]
- C.-Y. Kim [1]
- C.S. Hoi [1]
- Chang Li [1]
- Chao-Cheng Lin [1]
- Chen-Cheng Lin [1]
- Chen-Hsun Du [1]
- Chung-Yuan Kung [1]
- Cuiping Kang [1]
- D. Lee [1]
- D.-H. Kim [1]
- D.H. Baek [1]
- D.J. Thomson [1]
- D.S.H. Chan [1]
- Danyu Wang [1]
- Dapeng Wu [1]
- Denis Buttard [1]
- Deqing Mo [1]
- Dong Zhao [1]
- Dongyoung Kim [1]
- Duo-Sheng Chen [1]
- E. Bobeico [1]
- E. Centurioni [1]
- E. Vilamajó [1]
- Egbert Vetter [1]
- Emanuele Cornagliotti [1]
- Ernst Granneman [1]
- Erqing Xie [1]
- F. Cappelluti [1]
- F. Elsehrawy [1]
- F. Finger [1]
- F. van de Wiele [1]
- F.C. Treble [1]
- F.H.T. Vieira [1]
- Fuxin Zhong [1]
- G. Beaucarne [1]
- G. Golan [1]
- G.P. Mishra [1]
- G.S. Sahoo [1]
- Ganesh C. Patil [1]
- Gunnar Kohler [1]
- H. Choi [1]
- H.J. Kim [1]
- H.S. Park [1]
- Haifang Zhou [1]
- Hans-Peter Sperlich [1]
- Haris Mehmood [1]
- Hermann Schlemm [1]
- Himanshu Sekhar Sahu [1]
- Hong Zhang [1]
- Hongjie Jia [1]
- Hongkun Cai [1]
- Hsien-Seng Hung [1]
- Hsin-Wei Lu [1]
- See more See less
Filter by access type:
Here to determine the thermal stability of buffered layer organic solar cell (BL-OSC), the effect of post anneal treatment has been studied. To investigate the effect of post annealing, the organic solar cells (OSCs) are annealed at the 120°C for different time duration. It has been observed that the BL-OSC structure exhibits the better thermal stability. Further, as the authors vary the post-annealing time duration from 0 min to 20 min, the power conversion efficiency (PCE) in the case BL-OSC drops by ∼20%, whereas in conventional OSC, the PCE drops by ∼35%. This annealing dependent study shows that, in conventional OSC structure an increase in phase segregation between donor and acceptor molecules reduces exciton dissociation and charge separation, this leads to sharp increase in series resistance and significant reduction in fill factor of the device. Whereas in the case of BL-OSS, there is a minimum reduction in the fill factor, which also determines the superior carrier collection and low recombination on the elevated annealing conditions. Further, the experimental results show that, in comparison with the conventional OSC structure, inserting the pure P3HT interlayer between PEDOT:PSS (hole transport layer) and P3HT:PCBM (photoactive layer) improves the PCE of the device by 34%.
Different ratio incorporation of Ag/TiO2 core–shell nanowires (ATCSN) into TiO2 as an electron transport layer of perovskite solar cells (PSCs) is studied. This structure can prevent the formation of silver halides between perovskite and silver nanowire. It is found that because of the effective improvement of light absorption and separation of photo-generated electron–hole pairs, the introduction of ATCSN leads to increase of short current density and photoelectric conversion efficiency (PCE) of PSCs. 20 mg incorporation of ATCSN PSCs exhibits the best performance of PCE and a 17.7% increase is achieved compared to the control sample.
Surface passivation of silicon solar cells describes a technology for preventing electrons and holes to recombine prematurely with one another on the wafer surface. It increases the cell's energy conversion efficiencies and thus reduces the cost per kWh generated by a PV system. In the past few years, new tools have been developed to ensure low cost of ownership for high volume production of passivated silicon solar cells. Different deposition techniques (ALD, PECVD, APCVD) and different materials (SiO2, Al2O3, Si3N4) have been tested during the development process of more than 10 years. Now, the silicon solar cell manufacturing industry is picking up the concept of rear side passivation. The next generation silicon solar cells in production will be the PERC (Passivated Emitter and Rear Cell) type using all the reported achievements including novel tool concepts and process technologies. This timely overview of silicon solar cell surface passivation, written by the leading experts in the field, is a key read for students and researchers working with silicon solar cells, as well as solar cell manufacturers.
Solar energy is a cornerstone of the future global sustainable energy system. The book chapter outlines how performance and energy yield increase will have to evolve concurrently to make PV a major electricity source and how PERC-technology is an important milestone in achieving this.
In this book chapter the properties of Al2O3 based p+ surface passivation is described, focusing on the impact of deposition conditions, annealing sequence, capping layer material, Al2O3 thickness, and surface morphology.
The author provides a historical review of research into the atmospheric pressure chemical vapour deposition (APCVD) of Al2O3 for silicon surface passivation in solar cell devices, considering deposition temperature influence on excess carrier lifetime, film thickness and interface state density.
In this book chapter it is shown that Al2O3 deposition systems based on spatial ALD with wafer floatation are attractive for passivation of cSi solar cells in high-volume manufacturing. In principle, the throughput can be increased to 7,200 wafers/h; the limitation is not the ALD track, but the unloading automation.
The authors review developments in the use of PECVD in the growth of AlOx layers for solar cells. They consider the microwave PECVD and inductively coupled plasma PECVD methods, and the characteristics of layers grown by the 2 techniques, Si surface passivation, and solar cell applications.
The author provides a general background on atmospheric pressure chemical vapor deposition (APCVD) of Al2O3, from its origins to more recent research, focusing on surface passivation applications for solar cells and the composition and structure of the APCVD Al2O3-Si interface.
In this book chapter, the authors summarize the main developments and improvements within the last 25 years which enabled the industrialization of the lab-type PERC solar cell concept. In particular, we describe the historic development and current status of key industrial PERC manufacturing process steps such as the rear passivation layer, typically applying an AlOx/SiNy layer stack, as well as the local Al rear contact formation by laser ablation, Al screen printing and subsequent firing. At the end of this chapter, an outlook is provided on future development opportunities such as further efficiency increases and bifacial PERC applications.
Surface passivation of moderately doped and heavily doped p-type surfaces is of major importance to both p-type and n-type solar cells. Considering the practical importance and relevance of p-type Si surfaces, i.e. a moderately doped (undiffused) p-type Si surface and a heavily doped p±-type Si surface, this chapter focuses on the investigation of surface passivation using double-layer dielectric stacks. We study a positively charged dielectric stack (i.e. SiOx capped with SiNx) as well as a negatively charged dielectric stack (i.e., AlOx capped with SiNx).
The book chapter shows that surface passivation technologies have played a crucial role in the development of industrial silicon solar cells over the past 40 years, and they will continue to do so in the future. The authors describe a variety of surface passivation techniques that will help to take industrial silicon solar cells to even greater heights, ensuring ongoing reductions of the levelized cost of electricity (LCOE) from PV systems and their global deployment on a massive scale.
Over recent decades, surface-passivating properties of PECVD a-SiNx:H have been investigated extensively. These properties depend on the number of fixed charges (Qf) and interface density of states (Dit) and are in turn related to bulk and interface properties. In general, there is a positive correlation between Qf and Dit, which have opposite effects on the surface-passivating properties. For an optimal effective surface passivation, an optimization is therefore necessary. Higher Qf and Dit are found to correspond to a higher and deeper insertion of N in c-Si thereby increasing the concentration of these defects. This insertion is related to NH3 flow and temperature during plasma treatment. This technique for forming defect layers has been experimentally validated by EELS as well as high resolution TEM. MD simulation and ab initio DFT studies demonstrated the formation of defects and higher DOS in the bandgap for the same layer composition. Introduction of hydrogen was simulated with DFT as well and showed a lower DOS in the bandgap resulting in a better surface passivation. The effect of Qf at the interface on the passivating properties of a-SiNx:H applied to completed solar cells was proven as well and confirmed by PC1D device simulations.
The book chapter reviews the process of spatial Al2O3 atomic layer deposition (ALD). Aspects covered include: time-based versus spatial methods; proof of principle spatial ALD; spatial ALD applications; from the proof of principle to InPassion® LAB; transform from Lab to Fab-InPassion® ALD; second generation-InPassion® ALD; combining the stack layers.
This book chapter gives an overview of industrial microwave PE CVD reactors starting at details of the used linear plasma sources and showing then, that a system of modular equipment can be constructed, covering a wide range of wafer throughput and customized backside passivation layer systems.
To improve light absorption, in this study, the narrow band gap highly-ordered free-standing hydrogenated amorphous germanium nanoparticles (a-Ge:H NPs) were introduced into the CH3NH3PbI3−x Cl x films. Here, the NPs were fabricated by means of the radio frequency plasma enhanced chemical vapour deposition system. The effects of hydrogen dilution ratio (RH) on the microstructure and bonding configuration of a-Ge:H NPs were investigated by Raman, transmission electron microscopy and Fourier transform infrared spectroscopy measurements. As RH increases, an improvement in the structure order of a-Ge:H NPs was observed. Compared with the pure CH3NH3PbI3−x Cl x films, the light absorption of the hybrid a-Ge:H NPs/CH3NH3PbI3−x Cl x active layers was improved, and the surface coverage of the hybrid active layers nearly reached 100%. This new finding provided a novel way to solve the universal unfavourable surface coverage problem that existed in the ultrasonic spray-coating process. Meanwhile, compared with the device that is based on pure CH3NH3PbI3−x Cl x films, due to the enhanced light absorption in the visible range, a ∼14.6% enhancement in the power conversion efficiency was achieved based on the hybrid a-Ge:H NPs/CH3NH3PbI3−x Cl x active layers.
Copper (Cu)-doped cadmium sulphide (CdS) quantum dots (QDs) sensitised zinc oxide photoelectrodes have been fabricated for a solar cell (SC). For the synthesis of QDs, simple chemical methods have been adapted and the QDs were prepared on poly-vinyl alcohol capping agent. The influences of doping on structural properties of QDs have been studied using X-ray diffraction analysis and transmission electron microscopy images. Ultraviolet–visible absorption spectroscopy reveals an enhanced optical absorption in doped QDs. The photovoltaic performance of the Cu-doped CdS QDs was studied by measuring the current density–voltage (J–V) characteristics of the fabricated SC. An enhanced photo-conversion efficiency was observed in doped CdS QDs compared with the undoped QDs sensitised SC.
The objective of this study is to present an economic analysis (EA) of actual installed photovoltaic (PV) projects considering Gulf Cooperation Council countries climate conditions. The two analysed PV systems are commissioned in Kuwait and they were chosen to be the scope of this study since the availability of their characteristics. The first system is installed on a school and equipped with thin film (copper indium gallium selenide) solar modules of efficiency equal to 14% and the other system is installed on a commercial building and equipped with monocrystalline solar modules of efficiency equal to 17%. The EA consists of studying the financial parameters related to the two previous projects using two different calculation tools. One tool is developed and presented in this study that is the EA calculator and the other tool is the existing solar advisory model software. The two calculation tools’ results almost match with slight differences considered negligible, so the developed EA calculator is considered validated. As a conclusion, the impact of renewable energy (RE) costs on future investments in RE technologies and especially on PV projects is being evaluated.
In this Letter, the authors present a new analytical method for determining the parameter values for the single-diode model of photovoltaic (PV) panels. More specifically, the authors propose explicit equations for all the parameters of the model so that their values can be directly extracted from the data provided in the PV panel datasheet. The results show that the proposed method provides smaller errors between the calculated and experimental I–V curves than other analytical approaches.
Organic bulk heterojunction solar cell based on poly 3hexylthiophene (P3HT) and [6,6]-phenyl-C61-butyric acid methyl ester (PCBM) blend as photoactive layer had been electrically simulated and analyzed at different thickness using general-purpose photovoltaic device model (GPVDM) software. Conjugate polymer P3HT acted as an electron donor, whereby PCBM acts as an electron acceptor in the device. The electrical simulation is performed at three different thicknesses of 50 nm, 100 nm, and 200 nm with P3HT/PCBM blend and hetero-layer configurations, respectively. The simulation analysis clearly demonstrated that both device configurations exhibited current-voltage (I-V) characteristics with highest short-circuit current density (Jsc) value of 2.26 mA/cm2 with P3HT/PCBM of blend configuration at 200 nm thickness. However, an open-circuit voltage (Voc) and fill factor (FF) showed a constant value, which 0.55 V and 0.72 a.u., respectively, for both device configurations. The obtained value of solar cell parameters was then analysed and compared with experimental data. This simulation work strongly reveals that different thickness of photoactive material affects the electrical performance even in different organic solar cell configurations.
A widely used approach to reduce the charge recombination and improve the performance of a silicon based Schottky barrier solar cell (SBSC) is to use an interfacial layer between metal and Si. In the present work we have investigated the role of graphene oxide (GO) as interfacial layer for p doped Si (p-Si) based SBSC utilizing AZO (Aluminum doped ZnO) as transparent top contact. The not obvious compatibility of the different layers combined in the solar device results clear from the improvement of all the electrical parameters measured in the AZO/GO/p-Si solar cell respect to the simple AZO/p-Si device used as reference. In particular dark IV characterization put in evidence the majority carrier blocking properties of the GO in this type of structure, with an increment of 140 meV in the barrier height respect to the device without GO, resulting in a 100% enhancement in the final solar cell efficiency.
Solar cells made of single-crystalline silicon, as alternative energy sources, became the most widely used solar cells in recent years. The mainstream manufacturing approach is to process the cells from Si wafers, and then assemble these cells into photovoltaic (PV) modules. However, the direct conversion of solar energy into electricity using the photovoltaic effect suffers from low efficiency. Thus, increasing the conversion efficiency at low production costs becomes the main goal of solar cells manufacturers. One way to increase the efficiency of a solar cell is to use an ultra-wide layer of intrinsic semiconductor as the depletion region of a P-N junction. Computer simulation shows that an intrinsic layer of 1 μm thickness results in an increase of the photovoltaic conversion efficiency by 4.85% for conventional single-crystalline silicon P-N junction. In our work, we present a novel geometrical concept of a PIN structure for PV applications. The width of the intrinsic layer in our construction is 5-20 mm. Moreover, in our novel structure, the light irradiation acts directly on the active region of the PV cell, which enables bi-facial irradiation and results in ~28% conversion efficiency. A low-cost fabrication is ensured in our design due to a new manufacturing technology by eliminating some expensive processes, such as photolithography. The feasibility proof of the novel concept in mono-crystalline silicon solar cells is presented. We demonstrate simulation results and preliminary experimental results confirming our approach. Detailed computer simulations show that the voltage drop and accordingly the high and constant electric field within the intrinsic region of the structure take place for sufficiently small sizes of the region (up to 200 - 300 nm). With extension of the intrinsic region length the field becomes extremely uneven with peak values at the p-i and i-n junctions. The field strength falls from tens of thousands Volts per centimeter to hundreds of Volts per centimeter for 5 μm intrinsic zone and after 10 μm the field practically disappears. Analysis of the simulation results, electrons and holes concentration profiles, space charge and electric field distributions, brings the idea that the uncompensated charges of the donors and acceptors at the n-i and p-i junctions are the source of the built-in field in the intrinsic region. The simulation of the p-i-n structure equilibrium state was done by the Silvaco's ATLAS silicon device simulator.
The study proposes designs using 2D photonic crystal (PhC) structure-based thin film heterojunction gallium arsenide (GaAs) solar cell with a periodic pattern having PhC structure extends from top transparent conducting oxide (TCO) to inside the p-AlGaAs window layer placed just above the active layer of GaAs material in one design and in another PhC structure is etched only in TCO. The work presents the comparative analysis of the proposed structure with Lambertian light trapping limits and the planar cell, taken as reference. The study is also performed for double-layer anti-reflective coating (ARC) structure. The study presents the quantitative analysis of the effect of PhC structure in the performance of the design and how the effect varies with the thickness of absorption layer. It has been found that a considerable increase in efficiency has been achieved, especially for thinner active layers, demonstrating the advantage of a wavelength-scale, PhC-based structures for thin-film solar cells. The results have shown that PhC structure (etched till inside p-AlGaAs)-based solar cell exceeds the efficiency of the double ARC-based structure by more than 18% for 50 nm thin active layer cell. The parameters have been optimised and calculated by means of rigorous coupled wave analysis (RCWA).
Cadmium selenide (CdSe) thin films were prepared on indium tin oxide substrate by an alternating cold–hot method, in which cadmium nitrate solution was used as a cold deposition solution, while sodium selenite and potassium borohydride mixed solution was used as a hot deposition solution. The influences of the preparation conditions such as the concentration of Cd(NO3)2, the number of deposition cycle and the cycle time, on the photoelectric performance of the sample under simulated sunlight were explored. The results show that the CdSe thin film prepared under the reaction conditions of 0.06 mol/l Cd(NO3)2 at the tenth deposition cycle (30 s per cycle) reaches the highest photovoltage of 0.285 V. Under the simulated solar illumination, the open-circuit voltage and short-circuit currents are 0.419 V and 5.57 mA/cm2, respectively. X-ray diffraction indicates that the strongest diffraction peak at 42.215° of the (111) crystal plane is corresponding to 15.15 nm CdSe nanocrystals. Scanning electron microscopy observation shows that the thickness of the CdSe film is about 200 nm and the size of the spherical and uniformly dispersed nanocrystals is around 50 nm.
The work presents the design of a diffraction back grating for light-trapping in thin-film GaAs-based quantum dot solar cells. Uni-periodic and bi-periodic gratings made of off-theshelf almost transparent dielectric materials routinely used in photolithography are considered. Gratings are wave-optics simulated by rigorous coupled wave analysis. Optimizing the shape and geometrical aspect ratio of the grating, almost quadrupled photocurrent from quantum dots is demonstrated.
The surface passivation for InGaN/GaN multilayer solar cells was investigated, and it was confirmed that the device with an atomic-layer-deposited (ALD) Al2O3 passivation film showed high internal and external quantum efficiencies of 99 and 84%, respectively, along with a high energy conversion efficiency of 1.31% under a 1-sun air-mass 1.5 global illumination. The current−voltage characteristics indicated that the ALD Al2O3 film improved the surface electrical stability. The carrier lifetime measurements revealed that the ALD Al2O3 film reduced the surface carrier recombination rate and thereby contributed to the improvement of the solar cell performance in a short wavelength region.
In this paper, the effect of an intrinsic layer inside the PN junction of both top and bottom cell of InGaP/GaAs Double Junction solar cell is investigated using computational TCAD modeling tool. Inclusion of intrinsic layer shows better performance in comparison to other structures and produces high conversion efficiency of 29.72% (1sun), high shortcircuit current density and open circuit voltage. For this optimized cell structure, the maximum Jsc=13.65mA/cm2, Voc=2.44 V, fill factor (FF) = 89.08 are obtained under AM1.5G illumination. The detail of photo-generation rate of top as well as bottom cell has been investigated through the incident light of various wavelengths.
The rear point-contact fabricated through the laser-opening technique for mass production was applied on the photovoltaic cells. Laser opening, different layers for passivation (SiO2) and protection (SiN X ) were employed to investigate their impact on the performances of solar cells. The SiN X layer protects the SiO2 layer from being burnt through by aluminium paste at the co-firing step. A conversion efficiency (η) of 16.91% with an open-circuit voltage of 628 mV was obtained for the optimal cell, a stack structure with SiO2 and SiN X layers, which also achieves a lower contact resistance of 6.66 mΩ·cm2 and a higher light-beam-induced current of 80.77 mA/cm2. The optimal cell also showed longer lifetime and 3–4% increased quantum efficiency in the visible wavelength range. Therefore, the developed process has simplicity and reliability, is fast and cost-effective and could be applied to industrial applications.
A low-cost, highly reflective, liquid organic nanostructure silver conductor with superior conductivity, using back contact reflectors in amorphous silicon (a-Si) single-junction superstrate configuration thin-film solar cells produced using a non-vacuum screen printing process is proposed. The conductive paste is composed of Ag nanowires (Ag NWs) mixed with an Ag nanostructure (Ag NS) sheet. The paste is referred to as ‘Ag NWS’. A comparison of silver conductor samples with vacuum-system-sputtered silver samples indicated that the short-circuit current density (J sc) and the open-circuit voltage (V oc) of Ag NWS conductor cells exceeded 0.22 mA/cm2 and 66 mV, respectively. The Ag NWS conductor with back contact reflectors in solar cells was analysed using external quantum efficiency measurements to effectively enhance light-trapping ability in a long wavelength region (580–700 nm). The cells constructed using the optimised Ag NWS demonstrated an increase of approximately 6.1% in power conversion efficiency under AM 1.5 illumination. These results indicated that the Ag NWS conductor back contact reflector layer is a suitable candidate for high-performance a-Si thin-film solar cells.
Two advanced fabrication methods are introduced: the hydrogen peroxide (H2O2)-added chemical bath deposition technique and molybdenum (Mo) back-contact formation under 3 kW sputter power. The parameters of the short circuit current density (J SC) and conversion efficiency (η) were improved over standard cells when the ZnS buffer layer was deposited in the H2O2-added chemical solution. Otherwise, the fill-factor and η were best at 3 kW Mo sputtering power conditions. Advanced fabrication methods are realised to improve cell performance without modifying the chemical composition of the Cu(In,Ga)Se2 absorption layer.
The novel structure of a solar cell is presented that has the metal–oxide-semiconductor diode at the side wall of the power generation layer. The influence of the field-effect on the recombination of carriers is simulated and the increase of the conversion efficiency of the solar cell by the gate voltage application is discussed. In addition, the relationship between the effect of the gate voltage application on the conversion efficiency, the lifetime and the surface recombination velocity is discussed.
A start-up circuit, used in a micro-power indoor light energy harvesting system, is described. This start-up circuit achieves two goals: first, to produce a reset signal, power-on-reset (POR), for the energy harvesting system, and secondly, to temporarily shunt the output of the photovoltaic (PV) cells, to the output node of the system, which is connected to a capacitor. This capacitor is charged to a suitable value, so that a voltage step-up converter starts operating, thus increasing the output voltage to a larger value than the one provided by the PV cells. A prototype of the circuit was manufactured in a 130 nm CMOS technology, occupying an area of only 0.019 mm2. Experimental results demonstrate the correct operation of the circuit, being able to correctly start-up the system, even when having an input as low as 390 mV using, in this case, an estimated energy of only 5.3 pJ to produce the start-up.
A multi-layered film with a TiO2-based nanotubes/nanoparticles/nanotubes sandwich structure has been developed to increase light-harvesting efficiency by enhancing light scattering. Compared to a double-layered film of nanotubes/nanoparticles, the sandwiched film exhibited greatly improved light-absorption properties. An obviously improved total energy-conversion efficiency of 6.11% was obtained in the sandwiched film, which is 27.3, 46.1 and 213% higher than those of the double-layered film, nanoparticle film and nanotube film, respectively. A possible mechanism for the enhancement of light harvesting in the sandwiched film is proposed, whereby the observed enhancement is owing to effective scattering by the bottom layer and reflection of escaped light by the top layer.
TiO2 spindles with high crystallinity were synthesised by a two-step solvothermal reaction with the aid of diethylamine. Compared with Degussa P25, the dye sensitised solar cell (DSSC) based on a TiO2 spindles photoanode demonstrated superior characteristics including higher affinity to N719 dye, higher light scattering effect than P25, better conductance and longer recombination lifetime. Photovoltaic measurement indicated that the TiO2 spindles-based DSSC possesses higher short-circuit current density (Jsc) and open-circuit voltage (Voc), hence, a 29% higher overall photovoltaic performance (η) than that of P25 was achieved.
Optimum heat treatment processes for carbon nanotubes (CNTs) paste counter electrodes with better electrochemical performance are investigated. Half-cells were fabricated to examine the electrochemical properties of the CNT paste counter electrode. Proposed is a two-step heat treatment process and an optimum sintering temperature for CNT paste counter electrodes.
The authors simulate both conventional and doping superlattice GaInNAs solar cells. They show that for a conventional cell with 1 µm diffusion lengths the maximum possible efficiency is approximately 9.5% and for 0.1 µm diffusion lengths it is 6.5% as the device must be relatively thin. Doping superlattice structures with varying number of layers and different layer thicknesses are simulated to find the design which yields the highest efficiency. A high number of thin layers allow a high percentage of incident photons to be absorbed, and carrier separated increasing the short-circuit currents leading to efficiencies close to 12%.
InGaN pin homojunction solar cells with different In content (x=0.02/0.12/0.15) have been fabricated. The measured open-circuit voltages (Voc) are 2.24, 1.34 and 0.96 V, respectively. All the devices exhibit large fill factors of more than 64% and enhanced response in the short wavelength region, suggesting the high potential of InGaN-based pin homojunction solar cells.
This presentation discusses some key characteristics of polymers and several polymer-based electronic devices such as polymer light-emitting diodes, photovoltaic diodes, organic solar cells, field-effect transistor, and electrophoretic display. (31 pages)
Carbon nanotubes (CNTs) with different diameters as a counter electrode to fabricate dye-sensitised solar cells with high conversion efficiency are investigated. The CNT electrodes with large diameter demonstrated better redox reaction and higher energy conversion efficiency.
One of the major drawbacks of photovoltaic systems is the high generation cost. To address this problem, the US Defense Advanced Research Projects Agency initiated a study to create a thousand 10 cm2 solar cells with over 50% efficiency, providing 500 mW in full sunlight, with reasonable manufacturing costs. Called the Very High Efficiency Solar Cell (VHESC) program, it hopes to take advantage of recent advances in nanotechnology by using engineered biological molecules to guide the assembly of inorganic materials into regular 3D structures, with dimensional and assembly control unattainable using current technologies. The program also hopes to benefit from the recent introduction of tools and processes to design and cost-effectively fabricate small-feature, complex, broad-spectrum non-imaging optics.
The InP/InGaAsP double heterojunction (DH) solar cell to increase the short-circuit current is investigated. The InP/InGaAsP DH solar cell has been newly designed having a 1.12 eV InGaAsP absorption layer. Increases of 100% in short-circuit current and 50.18% in efficiency for the DH device are observed over the control sample.
(Ga,In)(N,As) could be a promising material for use in monolithic four-junction solar cells since it can be grown lattice-matched to substrates such as GaAs and Ge, and its bandgap of 1 eV is complementary to that of the three other semiconductors Ge, GaAs and (Ga,In)P. The growth by molecular beam epitaxy of (Ga,In)(N,As)-based solar cells is reported. It was checked by high-resolution X-ray diffraction that the 1-μm-thick (Ga,In)(N,As) layers were lattice-matched to GaAs. The spectral responses of the solar cells provide evidence that (Ga,In)(N,As) converts photons with energy down to 0.9 eV. The comparison with reference GaAs solar cells indicates, however, a degradation of the short-circuit current, revealing short minority-carrier diffusion lengths. A (Ga,In)(N,As) 2 mm×2.5 mm solar cell with a p–i (Ga,In)(N,As) n-GaAs structure delivers a 2.1 mA/cm2 short-circuit current and has an open-circuit voltage of 0.264 V under natural solar illumination (air mass ∼1.5).
A new gas-jet electron beam plasma enhanced chemical vapour deposition (GJEB PECVD) method for high-rate deposition of crystalline silicon films is presented. The method is based on the activation of initial gas molecules in an electron beam plasma and fast convective transfer of the radicals to a substrate by means of a supersonic free jet. Nanocrystalline, microcrystalline and polycrystalline Si film growth on different foreign substrates is investigated using morphological and optical analyses in dependence on the temperature of the substrate and its distance from the nozzle. It is shown that a middle range of substrate distance is required to avoid crystallinity damage by heavy ions while still keeping their effect on grain nucleation. In this case, well shaped crystalline grains embedded with a ‘highly ordered’ amorphous phase are found in Si films grown at a low temperature at the edge of crystalline growth.
Thin film polycrystalline silicon solar cells on foreign substrates are viewed as one of the most promising approaches to cost reduction in photovoltaics. To enhance the quality of the film, the use of ‘seeding layers’ prior to deposition of active material is being investigated. It has been shown that a phenomenon suitable to create such a seeding layer is the aluminium-induced crystallisation of amorphous silicon. Previous work mainly considered glass as the substrate of choice, thereby introducing limitations on the deposition temperature. Results concerning the application of such a technique to ceramic substrates (allowing the use of high-temperature CVD) are described. Also, the first reported results of a solar cell made in silicon deposited on these seeding layers are presented.
Measurements were made of conductance noise of a-Si:H and a-Si1−xGex:H in two different geometries: one where the current flow is transverse to the surface and the other where it is longitudinal to the surface. Because of the large change in sample resistance between the two geometries, it was not possible to measure both geometries at the same temperature. For both geometries, alloying with up to 40% Ge reduces the noise magnitude by several orders of magnitude over that found in a-Si:H. The decrease is incompatible with several popular noise models. Extrapolating the temperature trends for each geometry shows that it is possible that the noise observed in the transverse samples has the same origin as the higher frequency part of the double power law spectra observed in the longitudinal samples.
Pulsed plasma enhanced chemical vapour deposition (PECVD) involves modulation of standard 13.56 MHz RF plasma in the kilohertz range. This allows an increase in the electron density during the ‘ON’ cycle, while in the ‘OFF’ cycle, neutralising the ions responsible for dust formation in the plasma. The authors report the development of state-of-the-art nanocrystalline Si (nc-Si:H) materials using a pulsed PECVD technique with 220 crystallite orientation, grain size of ∼200 Å, low O concentration and a minority carrier diffusion length Ld of ∼1.2 μm. The crucial effects of the p/i interface and the incubation layer have been investigated and an efficiency of ∼7.5% for a single junction nc-Si:H p-i-n device has been achieved for an i-layer thickness of 1.4 μm, using non-optimised textured substrates.
The development of microcrystalline silicon (μc-Si:H) for solar cells has made good progress with efficiencies better than those of amorphous silicon (a-Si:H) devices. Of particular interest is the absence of light-induced degradation in highly crystalline μc-Si:H. However, the highest efficiencies are obtained with material which may still include a-Si:H regions and light-induced changes may be expected in such material. On the other hand, material of high crystallinity is susceptible to in-diffusion of atmospheric gases which, through adsorption or oxidation, affect the electronic transport. Investigations are presented of such effects concerning the stability of μc-Si:H films and solar cells prepared by plasma-enhanced chemical vapour deposition and hot wire chemical vapour deposition.
A review of recombination in silicon thin-film solar cells studied by means of electrically detected magnetic resonance (EDMR) is presented. It is shown that the EDMR results in μc-Si:H p-i-n solar cells can be described by a simple diffusion model that was developed for crystalline silicon p-n junctions assuming that recombination is dominated by dangling bonds in the space charge region. The results are compared to a-Si:H p-i-n cells and discussed in a recombination model involving the excited states of charged dangling bonds.