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Devices modeling

Fig. 5. Device model for an MIS photodiode, the basic building block of the CCD photodetector. The depletion region is generated by the battery... Fig. 5. Device model for an MIS photodiode, the basic building block of the CCD photodetector. The depletion region is generated by the battery...
Experimental part was provided by device Model Knauer-Compact with UV-detector (b=3 mm) at 250 nm and column Spherisorb-ODS-2 (250x4,6 mm). Sample volume was 1-2 p.1 injected by Reodyne 7725. Concentration range was 0.4-0.5 mg/ml for solutions of studied substances in DMSO. The organic modificator concentration range was 75-85 % w for methanol and 40-60 % w for acetonitrile in eluent (flow rate -1 ml/min). [Pg.286]

The device model describes transport in the organic device by the time-dependent continuity equation, with a drift-diffusion form for the current density, coupled to Poisson s equation. To be specific, consider single-carrier structures with holes as the dominant carrier type. In this case,... [Pg.186]

The hole current in this LED is space charge limited and the electron current is contact limited. There are many more holes than electrons in the device and all of the injected electrons recombine in the device. The measured external quantum efficiency of the device is about 0.5% al a current density of 0.1 A/cm. The recombination current calculated from the device model is in reasonable agreement with the observed quantum efficiency. The quantum efficiency of this device is limited by the asymmetric charge injection. Most of the injected holes traverse the structure without recombining because there are few electrons available to form excilons. [Pg.190]

One has to consider that in Eqs. (9.15)—(9.17) the mobility /t occurs as a parameter. As it will be pointed out below, // shows a characteristic dependence on the applied electric field typical for the type of organic material and for its intrinsic charge transport mechanisms. For the hole mobility, //, Blom et al. obtained a similar log///,( ) const. [E dependency [88, 891 from their device modeling for dialkoxy PPV as it is often observed for organic semiconductors (see below). [Pg.474]

A device model to describe two-carrier structures is basically similar to that used for one carrier structures except that continuity equations for both earner types are solved. The additional process that must be considered is charge carrier recombination. The recombination is bimolecular, R=y(np), where the recombination coefficient is given by 43)... [Pg.502]

Specific details to enable the affected product to he easily identified e.g. type of device, model name and number, batch/ serial numbers of affected devices and part or order number. [Pg.272]

Figure 1. The tunneling of a single electron (SE) between two metal electrodes through an intermediate island (quantum dot) can be blocked of the electrostatic energy of a single excess electron trapped on the central island. In case of non-symmetric tunneling barriers (e.g. tunneling junction on the left, and ideal (infinite-resistance) capacitor on the right), this device model describes a SE box . Figure 1. The tunneling of a single electron (SE) between two metal electrodes through an intermediate island (quantum dot) can be blocked of the electrostatic energy of a single excess electron trapped on the central island. In case of non-symmetric tunneling barriers (e.g. tunneling junction on the left, and ideal (infinite-resistance) capacitor on the right), this device model describes a SE box .
For either conventional polycrystalline semiconductors or nanotubes and nanowires to be successful, the development of model and simulation tools that can be used for device and circuit design as well as for predictive engineering must be available. Since these devices are not necessarily based on single wires or single crystals, but rather on an ensemble of particles, the aggregate behavior must be considered. Initial efforts to provide the necessary physical understanding and device models using percolation theory have been reported.64,65... [Pg.19]

Simple switches that can be manually activated can be considered a fire alarm device. Models are used which normally require the use of positive force, i.e., to avoid accident and fraudulent trips. Fire alarm switches normally can only be reset by special tools in order to trace the source of the alarm, however sophisticated data reporting systems with addressable data collection may make this requirement obsolete. [Pg.178]

MH Lu and JC Sturm, Optimization of external coupling and light emission in organic light-emitting devices modelling and experiment, J. Appl. Phys., 91 595-604, 2002. [Pg.560]

Davids PS, Campbell IH, Smith DL (1997) Device model for single carrier organic diodes. J Appl Phys 82 6319... [Pg.65]

Ryzhii V, Ryzhii M, Satou A et al (2009) Device model for graphene bilayer field-effect transistor. J Appl Phys 105 104510... [Pg.174]

The mastication equipment most commonly employed is standard rubber instrumentation such as roll mills, internal mixers, extruders or laboratory devices modeled on them (e.g., a single-rotor internal masticator described by Wilson and Watson (43), die model improved by Kargin and coworkers (11) and the Brabender plastograph). [Pg.30]

In 1983, SPICE 2G.6 was released and remained the industry standard for many years. Motivated by the increased use of UNIX workstations and superior programming tools, SPICE 2 was converted into the C programming language and released as SPICE 3. Although SPICE 3 is not entirely backward compatible with SPICE 2, the new features far outweigh this drawback. SPICE 3 has a technical advantage of being readily modified because it is written in C. SPICE 3 also offers more and improved device models and analysis functions. [Pg.7]

M. J. Ward, Asymptotic Methods in Semiconductor Device Modeling, Ph.D. thesis, Caltech, Pasadena, CA, 1988. [Pg.159]

At that time most semiconductor transport studies concentrated upon the engineering aspects of specific semiconductor devices. This trend was later joined by an intensive development of numerical methods for semiconductor device modelling. In parallel, the amount of research on macroscopic aspects of ionic transport decreased with this area s acquiring a reputation of being somewhat short of surprises, with the features of electro-diffusion regarded as almost identical to those of linear diffusion. [Pg.263]

M. S. Mock, An example of nonuniqueness of stationary solutions in semiconductor device models, COMPEL, Internat. J. Comp. Math., 1 (1982), pp. 165-174. [Pg.264]

Heat transfer involving non-Newtonian fluids has not been studied in rotating devices. Models have been developed for gravity-driven heat transfer for power-law fluids (46). These models may be useful as a starting point to evaluate performance in higher-gravity fields. [Pg.57]

K. Lee, M. Shur, T.A. Fjeldly, T. Ytterdal, Semiconductor Device Modeling for VLSI, Prentice-Hall, Englewood Cliffs, NJ, 1993, p. 500-504. [Pg.342]

From the previous results it is reasonable to propose the following device model for a bulk hetero junction solar cell (Fig. 5.17) ... [Pg.183]

Actually, research by modelling is more and more extensively used in many applications because complex devices models, composed of different elements, can be made by assembling models the solutions of which are frequently available. This behaviour presents an impressive growth and is sustained by the extraordinary developments in numerical calculations and by the implementation of commonly used computers with a high capacity and calculus rate. Nevertheless, modelling based on the equations of transport phenomena cannot be applied to every system, because they can present some limitations, which are summarized here. [Pg.48]

Sano, N., Hiroki, A. and Matsuzawa, K. (2002) Device Modeling and Simulations Toward Sub-10 nm Semiconductor Devices. IEEETrans. Nanotechnd., 1,63-71. [Pg.329]


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