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NETWORK MANAGEMENT in NET Encode QR Code in NET size, image with visual basicnet barcode sdk directivity antennas and antenna pointer tracking, the level of multiple access interference (MAI and the required transmitted power are reduced In order to exploit the available propagation diversity signals arriving from different directions (azimuth , elevation ) and delay are combined in a three-dimensional ( , , ) RAKE receiver This is expected to signi cantly improve the system performance In this section we present a systematic mathematical framework for capacity evaluation of such a CDMA network in the presence of implementation imperfections and a fading channel The theory is general and some examples of a practical set of channel and system parameters are used as illustrations. As an example, it was shown that, in the case of voice applications and a two-dimensional (4 antennas 4 multipaths) RAKE receiver, up to 90 % of the system capacity can be lost due to the system imperfections Further elaboration of these results, including extensive numerical analysis based on the offered analytical framework, would provide enough background for understanding of possible evolution of advanced W-CDMA and MC CDMA towards the fourth generation of mobile cellular communication networks The physical layer of the third generation of mobile communication system (3G) is based on wideband CDMA The CDMA capacity analysis is covered in a number of papers and recently has become a subject in standard textbooks [2 8] The effect of more sophisticated receiver structures (like multiuser detectors MUD or joint detectors) on CDMA or hybrid systems capacity has been examined in [9 13]. It is interesting to compare this with the result of the ion-trap laser simulations, as the latter showed both the ordinary laser threshold and the second threshold [444] We can understand why this happens by looking at how the time scales compare in the two cases In the ion-trap laser proposal [444], the best realistic values given the constraint of finding a suitable ion for trapping, were g ~ 148 MHz, t-;a~ ~ 1 MHz, and 'I'll ~ 106 MHz Notice how the atomic decay rate 'I'll is dangerously close to the Rabi frequency In the one-and-the-same atom laser experiment [436], however, g ~ 16 MHz, t-;a~ ~ 42 MHz, and 'I'll ~ 26 MHz So whereas in the ion-trap laser proposal the saturation photon number was no ~ 02 and the critical atom number No ~ 0. The results in H m l inen et al [9] show roughly twofold increase in capacity with MUD a aa ef ciency 65 % compared with conventional receivers The effect of the fractional cell load on the coverage of the system is presented in [10] The coverage of MUD-CDMA uplink was less affected by the variation in cell loading than in conventional systems References [11] and [12] describe a CDMA system where joint data estimation is used with coherent receiver antenna diversity This system can be used as hybrid multiple access scheme with TDMA and FDMA component In Manji and Mandayam [13] signi cant capacity gains are reported when zero forcing multiuser detectors are used instead of conventional single-user receivers In most of the references it has been assumed that the service of interest is low rate speech. 09, in the Caltech experiment no ~ 001 and No ~ 008 Another important experimental result is the demonstration of sub-Poissonian photon statistics The physics here is the same as for a multiatom laser [275, 354, 459, 504, 505, 521, 522] This is a consequence of the atomic and field dynamics having similar time scales that do not allow the adiabatic elimination of the nonlasing atomic levels involved in the pumping schemel! [74] Without strong coupling, however, it is not possible to get sub-Poissonian photon statistics with a single atom in this way [459] So this result provides firm evidence that the Caltech experiment has indeed achieved the strong-coupling regimeRelated: ASPNET Data Matrix Generator , NET UPC-E Generation , Create UPC-A Java. open source ocr software windows 10 Easy Screen OCR - Free Download - Tucows Downloads
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