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[22] Kari Sipil , Zhi-Chun Honkasalo, Jaana Laiho-Steffens, Achim Wacker, Estimation of Capacity and Required Transmission Power of WCDMA Downlink Based on a Downlink Pole Equation, Proceedings of IEEE Vehicular Technology Conference 2000 Spring, Tokyo, Japan, May 2000, pp 1002 1005 [23] Stefan Brueck, Performance Characterisation of WCDMA dedicated Traffic Channels based on Node B Transmit Power and Pilot Measurements, Fifth IEE International Conference on 3G Mobile Communication Technologies (3G 2004), pp 480 484 [24] Toni Janevski, Traffic Analysis and Design of Wireless IP Networks, Artech House, 2003 [25] AM Viterbi and AJ Viterbi, Erlang Capacity of a Power Controlled CDMA System, IEEE Journal on Selected Areas in Communications, vol 11, no 6, August 1993, pp 892 900 [26] J Lee, L Miller, CDMA System Engineering Handbook, Artech House, 1998 [27] D Molkdar, S.

Burley, On the Nature of UMTS Circuit-Switched Capacity Figures Obtained Through Monte Carlo System-Level Simulation, fifth IEE International Conference on Mobile Communication Technologies (3G 2004), London, UK, 18 20 October 2004 [28] Andreas M der, Dirk Staehle, Analytical Modelling of the WCDMA Downlink Capacity in Multi-Service Environment, Research Report Series, Report Number 330, April 2004, http://www3informatikuniwuerzburgde/TR/tr330pdf [29] Andreas M der, Dirk Staehle, Uplink Blocking Probabilities in Heterogenous WCDMA Networks considering Other-Cell Interference, Research Report Series, Report Number 333, May 2004, http://www3informatikuniwuerzburgde/TR/tr333pdf [30] Maciej J Nawrocki, Tadeusz W Wieckowski, Optimal Site and Antenna Location for UMTS Output Results of 3G Network Simulation Software, 14th International Conference on Microwaves, Radar and Wireless Communications, MIKON-2002, 2002..

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Once the site is ready for installation, an application needs to be lodged for the allocation of radio channels for each of the PMP sectors and PTP links. The application may be to an internal application to the radio planning department (this is usual in the case that a `block' allocation of spectrum has already been made to the operator by the national radio agency in the given geographic region this is the most common way of allocating spectrum to PMP operators, as we discussed in 9). Alternatively, it may be necessary to apply to the national radio agency for a radio channel for each individual link. This is the normal manner of allocation of spectrum for point-to-point radio systems. The national radio agency thus assumes the overall coordination of frequency re-use planning for PTP. The application may take anything from a few days up to about four weeks, depending upon whether the applicant is known to the radio agency, and depending upon the availability of resources and level of demand.

Case "PAS" '-- PASS '-- Logged in! Get the messages. szTemp1 = UCase$(ReceiveData) szTemp2 = UCase$(mszUser) & " HAS" szTemp3 = "MESSAGE" nPos = InStr(szTemp1, szTemp2) If nPos Then nPos2 = InStr(szTemp1, szTemp3) If nPos2 Then nNumMessages = Val(Mid$(szTemp1, _ nPos + Len(szTemp2), nPos2 - _ (nPos + Len(szTemp2)))) frmMain.Caption = Str$(nNumMessages) & _ " New Messages" '-- Once we have the number of messages ' send the TOP command to retrieve the ' header (once for each message). ' nCurMessage keeps track of the message ' we're currently reading the header of. nCurMessage = 1 Screen.MousePointer = vbHourglass SendPOP3Command dsSocket1, "TOP 1 0" End If End If Case "QUI" '-- QUIT '-- Reset the last command mszCommand = "" Case "RET" '-- RETR '-- Here comes the message nCommandMode = False Screen.MousePointer = vbHourglass Case "RSE" '-- RSET mszCommand = "" Case "STA" '-- STAT

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NOTE The phase velocity of electromagnetic waves in each of these media is up = / . Thus, u p = c r for a nonconducting medium, but u p = ( c r ) 2 for a strongly conducting medium.

and the transit time of the light through the external cavity is . Since the rate equation only includes the effect of a single round trip through the external cavity, this model is inherently limited to the case of weak optical feedback (i.e. small values of ) where the contribution to the E-field rate-equation from the second and subsequent round trips can be ignored. To obtain the feedback coefficient given in Equation (2.2) we must first determine the effective reflectivity of the laser facet subject to the optical feedback. Figure 2.1 shows the external cavity configuration under consideration. If the field incident on the right laser diode facet (reflectivity R2 ) is given by, Ei ei 0 t , then providing we only consider one reflection of the field in the external cavity, the total reflected field from that facet is given by: Er e i

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