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Other Solar Cells

Harold J. Hovel, Introduction Carrier Collection, Spectral Response, and Photocurrent Solar Cell Electrical Characteristics Efficiency Thickness Other Solar Cell Devices Radiation Effects Temperature and Intensity Solar Cell Technology... [Pg.648]

The poly-Si films obtained by ALILE process always show p-type behavior. On high temperature resistant foreign substrates, the p-type poly-Si can be transferred to n-type poly-Si by overdoping, e.g., by phosphorous diffusion at 950°C [68], This allows for other solar cell configurations (e.g., substrate/ n+-type ALILE seed layer/n-type absorber/p+-type emitter). [Pg.213]

Or, take a reading for one cell (this will be your control) under the artificial light at a specific distance. Then, take the other solar cells and see if they are close in output to the control cell. This will give a relative comparison to a cell which you know has the output that you need. [Pg.20]

The SBSC in common with other solar cells is a low impedance device and as such should possess a low series resistance. The three main factors which contribute to increased series resistance are contact resistance, sheet resistance of the semitransparent metal layer forming the Schottky barrier and bulk resistance of the semiconductor substrate. [Pg.95]

Hyperpure silicon can be doped with boron, gallium, phosphorus, or arsenic to produce silicon for use in transistors, solar cells, rectifiers, and other solid-state devices which are used extensively in the electronics and space-age industries. [Pg.34]

Mercury Telluride. Compounds of mercury with tellurium have gained importance as semiconductors with appHcations in infrared detection (9) and solar cells (10). The ratio of the components is varied, and other elements such as cadmium, zinc, and indium are added to modify the electronic characteristics. [Pg.114]

A photovoltaic (PV) solar power system is a complete electrical source that uses solar cells to directly convert light energy into electricity. The system can be self-contained and completely autonomous or it can work in tandem with other conventional fuel-based sources of power to offer robust power availabihty. [Pg.466]

Because of the high functional values that polyimides can provide, a small-scale custom synthesis by users or toU producers is often economically viable despite high cost, especially for aerospace and microelectronic appHcations. For the majority of iudustrial appHcations, the yellow color generally associated with polyimides is quite acceptable. However, transparency or low absorbance is an essential requirement iu some appHcations such as multilayer thermal iusulation blankets for satellites and protective coatings for solar cells and other space components (93). For iutedayer dielectric appHcations iu semiconductor devices, polyimides having low and controlled thermal expansion coefficients are required to match those of substrate materials such as metals, ceramics, and semiconductors usediu those devices (94). [Pg.405]

In most cases, CVD reactions are activated thermally, but in some cases, notably in exothermic chemical transport reactions, the substrate temperature is held below that of the feed material to obtain deposition. Other means of activation are available (7), eg, deposition at lower substrate temperatures is obtained by electric-discharge plasma activation. In some cases, unique materials are produced by plasma-assisted CVD (PACVD), such as amorphous siHcon from silane where 10—35 mol % hydrogen remains bonded in the soHd deposit. Except for the problem of large amounts of energy consumption in its formation, this material is of interest for thin-film solar cells. Passivating films of Si02 or Si02 Si N deposited by PACVD are of interest in the semiconductor industry (see Semiconductors). [Pg.44]

In addition, other utiUties are installing estabUshed solar cells in a growing number of tests that may lead to a mass market. The studies may indicate the extent to which solar cells can be used to avoid installation costs for new distribution lines between conventional power plants and remote customers buildings. Also, among other objectives, PV cells may provide an economical means of helping to supply demand during peak summer periods in northern climates. [Pg.105]

Many grades of interlayer are produced to meet specific length, width, adhesion, stiffness, surface roughness, color (93,94), and other requirements of the laminator and end use. Sheet can be suppHed with vinyl alcohol content from 15 to about 23 wt %, depending on the suppHer and appHcation. A common interlayer thickness for automobile windshields is 0.76 mm, but interlayer used for architectural or aircraft glaring appHcations, for example, may be much thinner or thicker. There are also special grades to bond rear-view mirrors to windshields (95,96) and to adhere the components of solar cells (97,98). Multilayer coextmded sheet, each component of which provides a separate property not possible in monolithic sheet, can also be made (99—101). [Pg.453]

Fig. 1. The energy levels in a semiconductor. Shown are the valence and conduction bands and the forbidden gap in between where represents an occupied level, ie, electrons are present O, an unoccupied level and -3- an energy level arising from a chemical defect D and occurring within the forbidden gap. The electrons in each band are somewhat independent, (a) A cold semiconductor in pitch darkness where the valence band levels are filled and conduction band levels are empty, (b) The same semiconductor exposed to intense light or some other form of excitation showing the quasi-Fermi level for each band. The energy levels are occupied up to the available voltage for that band. There is a population inversion between conduction and valence bands which can lead to optical gain and possible lasing. Conversely, the chemical potential difference between the quasi-Fermi levels can be connected as the output voltage of a solar cell. Fquilihrium is reestabUshed by stepwise recombination at the defect levels D within the forbidden gap. Fig. 1. The energy levels in a semiconductor. Shown are the valence and conduction bands and the forbidden gap in between where represents an occupied level, ie, electrons are present O, an unoccupied level and -3- an energy level arising from a chemical defect D and occurring within the forbidden gap. The electrons in each band are somewhat independent, (a) A cold semiconductor in pitch darkness where the valence band levels are filled and conduction band levels are empty, (b) The same semiconductor exposed to intense light or some other form of excitation showing the quasi-Fermi level for each band. The energy levels are occupied up to the available voltage for that band. There is a population inversion between conduction and valence bands which can lead to optical gain and possible lasing. Conversely, the chemical potential difference between the quasi-Fermi levels can be connected as the output voltage of a solar cell. Fquilihrium is reestabUshed by stepwise recombination at the defect levels D within the forbidden gap.
In inaccessible regions where an impressed current installation is not sufficiently close to a low voltage supply, the protection current can be supplied from batteries, thermogenerators, and if there is sufficient radiation from the sun, solar cells. Wind generators and diesel units, on the other hand, are less suitable because of the maintenance necessary for continuous operation. [Pg.237]

The polymer may be regarded in these applications as a form of photoresistor (see Chapter 14) and is now finding other applications in this area. It has been used in holography and in the manufacture of printing plates whilst it has also been suggested for use in solar cells and for measuring photoelectric resistance. [Pg.474]

The chemical and electronic properties of elements at the interfaces between very thin films and bulk substrates are important in several technological areas, particularly microelectronics, sensors, catalysis, metal protection, and solar cells. To study conditions at an interface, depth profiling by ion bombardment is inadvisable, because both composition and chemical state can be altered by interaction with energetic positive ions. The normal procedure is, therefore, to start with a clean or other well-characterized substrate and deposit the thin film on to it slowly at a chosen temperature while XPS is used to monitor the composition and chemical state by recording selected characteristic spectra. The procedure continues until no further spectral changes occur, as a function of film thickness, of time elapsed since deposition, or of changes in substrate temperature. [Pg.30]


See other pages where Other Solar Cells is mentioned: [Pg.92]    [Pg.152]    [Pg.274]    [Pg.128]    [Pg.3]    [Pg.502]    [Pg.307]    [Pg.307]    [Pg.122]    [Pg.229]    [Pg.293]    [Pg.293]    [Pg.388]    [Pg.92]    [Pg.152]    [Pg.274]    [Pg.128]    [Pg.3]    [Pg.502]    [Pg.307]    [Pg.307]    [Pg.122]    [Pg.229]    [Pg.293]    [Pg.293]    [Pg.388]    [Pg.2888]    [Pg.245]    [Pg.467]    [Pg.468]    [Pg.474]    [Pg.507]    [Pg.360]    [Pg.362]    [Pg.532]    [Pg.21]    [Pg.389]    [Pg.433]    [Pg.433]    [Pg.240]    [Pg.269]    [Pg.280]   


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