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the load and the exural rigidity of the lithosphere. The latter, in turn, is dependent on the effective elastic thickness of the lithosphere, Te (Section 2.11.4). Thus, if the magnitude of the load can be calculated and the amount of exure determined, Te may be deduced. However as indicated above (Section 2.11.6), Te may be determined more generally from the spectral analysis of gravity and topographic data. Results obtained by applying this technique to oceanic areas are very consistent. They reveal that the elastic thickness of oceanic lithosphere is invariably less than 40 km and decreases systematically towards oceanic ridges (Watts, 2001) (Fig. 2.38). By contrast, the results obtained for continental areas vary from 5 to 110 km, the highest values being obtained for the oldest areas the Precambrian cratons. However, McKenzie (2003) maintains that if there are sub-surface density contrasts that have no topographic expression, so-called buried or hidden loads, the technique yields an overestimate of the elastic thickness. Such loads are thought to be more common in continental areas, particularly in the cratons, because of their thick and rigid lithosphere. In oceanic areas loads are typically super-

However, the situation is not when the client is located on a different computer to the server In this situation, the rendezvous may better for the following reasons the client is remote from be If the monitor, then a protocol such as Java s Remote Method Invocation ) must (WI be used to transfer the client s invocation to the remote computer on which the monitorislocatedAtthislocation, M I createsa newthreadtoperformthe invocation onthemonitoronbehalf of theclientThisthreadcreationisnot required by a remote rendezvous We have used the issueof efficiency to focus the differences in implementaon tionbetweenrendezvousandmonitormethodinvocationHowever,wecan model programsat a sufficiently abstract level that the model can be implemente by either mechanism For example, the model for the bounded buffer presented in 5 capturesthebehavior of boththemonitor ~ p l e m e n t a t i o ~ the and rendezvous im~lementationwehaveoutlinedinthissectionThisillustratesa more general point.

single symbol might have multiple bits in error - it still is a single symbol error from the perspective of the RS decoder. A single symbol might have up to m bits in error. Under the best of circumstances then, when all the errors affect adjacent bits of a symbol, a RS code may correct up to mt bits in error. This means that RS codes are naturally effective for transmitting over bursty binary channels: since bursts of errors tend to cluster together, there may be several binary errors contributingto a single erroneous symbol. As an example [203, p. 2781, a burst of length 3m 1 cannot affect more than 4 symbols, so a RS code capable of correcting 4 errors can correct any burst of length 3m 1. Or any burst of length m 1 cannot affect more than two bytes, so the 4-error correcting code could correct up to two bursts of length m 1. In general, a t-error correcting RS code over GF(2'") can correct any combination of t 1 U m - 2)/mJ

The modeling techniques we are using to describe and analyze concurrent programs are not restricted to programs implemented in Java They can be used to model message-passing programs with equal facility..

The addition of Flash Text to Dreamweaver goes a long way toward solving one of the Web designer s most perplexing problems: how to achieve good-looking text that uses non-standard fonts. While standard HTML text allows font families a series of fonts offered in hopes that one of them is installed on the user s system few designers stray outside of tried and true options such as Arial, Helvetica, and Times New Roman for the majority of their content. This is especially grating to print designers coming to the Web who rely on typography as a primary design tool. The advent of Dynamic HTML promised to bring a wider selection of typefaces with so-called dynamic font technology, but lack of built-in cross-browser support for any one system dashed those hopes.

Blase, Impurity dimers in superconducting B doped diamond: Experiment and rst principles calculations; Phys Rev B , 74 (2006) 094509 [73] WL Wang, M Polo, G Sanchez, J Cifre, J Esteve, Internal stress and strain in heavily boron-doped diamond lms grown by microwave plasma and hot lament chemical vapor deposition, J Appl Phys, 80 (1996) 1846 [74] S Kajihara, A Antonelli, J Bernholc, R Car, Nitrogen and potential n-type dopants in diamond, Phys Rev Lett, 66 (1991) 2010 [75] E Gheeraert, S Koizumi, T Teraji, H Kanda, M Nesladek, Electronic states of phosphorous in diamond, Diamond and Related Materials, 9 (2000) 948 [76] S Koizumi, M Suzuka; n-Type doping of diamond; Phys Stat Sol (a), 203 (2006) 3358 3366 [77] R Li, A molecular dynamics study of boron and nitrogen in diamond; Solid State Commun, 135 (2005) 155 [78] S Koizumi, K Watanabe, M Hasegawa, H.

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