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In this chapter, we review the various modeling and simulation techniques used for semiconductor devices, with primary emphasis on those that are useful for ULSI (MOSFETs and BJTs). 1,2 We examine these simulation methods at different levels of complexity and accuracy. First we discuss a fundamentally quantum mechanical picture of what is a complicated, many-body electron transport problem. We shall see what the various approximations are that enable one to reduce this problem to a single-electron Schr6dinger equation, with an "effective" mass to quantummechanically account for the complicated interactions of the electrons with the periodic lattice potential. These electrons with an effective mass, different from the true mass, will be shown to respond to the external potential according to Newtonian dynamics, except for occasional scattering mechanisms. This forms the base of what is called semiclassicalelectron dynamics.3 The carrier concentrations are generally determined on the basis of a parabolic density of states and the quantum-statistical Fermi-Dirac (FD), or classical Maxwell-Boltzmann (MB) distribution function. One can then simulate devices in the semiclassical regime using a single-particle picture with statistical Monte Carlo (MC) techniques. Alternatively, one can form a collective picture of carrier transport based on the evolution of the distribution function according to semiclassical dynamics, which is the Boltzmann transport equation (BTE). Next we will show, with examples drawn from MOSFETs and BJTs, how this treatment simplifies to the conventional device simulation formalism under certain conditions. 1 ,2 Conventional modeling is based on the self-consistent solution of the Poisson equation with the carrier (electron and hole) continuity equations and the drift diffusion equations for current transport. What will become clear from that discussion is how the approximations implicit in conventional device

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A method for non-invasive determination of the platinum concentration in tumours is desirable in order to collect more information on cisplatinum uptake, retention and metabolism in tumours and risk organs A plane polarised XRF system for platinum measurement in head and neck tumours was developed and optimised by Monte Carlo methods (Ali et al, 1998a,b; Kadhim et al, 2000) A radiotherapy treatment unit operated at 220 kV, a lter and a bi-layer polariser produced a detection limit of 56 g/g for a tumour depth of 20 mm and a skin dose of 3 mGy This system is similar to that developed by Jonson et al (1985) and used for platinum measurements in tumours and kidneys after cisplatinum therapy This subchapter reviews some of the methods used for quanti cation of various elements using in vitro and in vivo methods.

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Nondestructive in vitro XRF methods are well established and the detection limits imply that low concentrations of many elements can be measured in samples of minerals, food, body uids, tissue specimen, etc Issues of medical interest include studies of heavy elements in blood, urine, sweat, skin, hair, teeth, biopsies of tissues and organs, breathing air and drinking water Carcinogenic and anti-tumour substances as well as elements causing allergic reactions have been studied Due to a decreased use of lead in petrol and decontamination of lead-based paint, although taking time and with delayed effects, lead concentrations may decrease over the coming decades On the other hand, elements like palladium and cadmium may become more important due to the use of automobile catalysors and long-term use of fertilisers in modern agriculture, respectively Epidemiological studies of elements like calcium may be of interest in order to establish presumed relations with coronary failure.

Ancient bones, studied in connection with prehistoric nds of eg pottery, give us ideas of lead intake a long time ago Progress in the in vivo eld has produced original techniques for measuring the toxic.

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When set to on, the arithabort database setting will abort the data process if an arithmetic error occurs, such as data overflow or divide-by-zero. If set to off, then only a warning message is passed if an arithmetic error occurs, and the data process is able to proceed. To set arithmetic abort in code, do the following:

and blue components of a picture could indeed be reduced to less than a quarter of their original full bandwidth without losing any apparent resolution. It was easy to see that the fine structure of an image actually comes from the underlying high resolution luminance component of the picture, which is almost identical to the spectral shape of the green color channel, which is all that blackand-white receivers ever display. Color sets, then, need to receive only low-resolution red and blue picture components and add them to the sharp green picture to get the full high-resolution color effect. It is interesting to note that a field-sequential color system can never take advantage of this great economy of spectrum utilization since each of its color components has only the one wide-band video channel to travel through, whether the accompanying high-frequency color components can be seen by human eyes or not. Just as we were getting these ideas together in early 1949, the FCC notified RCA that it was issuing a request for comparative tests of the two main competing color television systems, CBS s field-sequential and RCA s compatible/simultaneous system. We were to make our presentations before them in Washington, DC, starting in October of that year. RCA was thus invited to prove immediately that its promising plan for a completely electronic and fully compatible color television system was indeed feasible and close to realization.

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