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electron energies can be computed. MC ,,imulations are extremely powerful because it is possible to incorporate more detailed bandstructure information (and consequently density-of-states informaton), and wavevector-dependent scattering rates than is possible analytically, or even with the solution of the BTE. One problem, however, with such brute-force numerical techniques is the numerical noise or scatter introduced. Generally speaking, the noise is inversely proportional to the square root of the number of particles simulated. There is, thus, a tradeoff between speed, which obviously goes down with increasing particle number, and accuracy, which improves with particle count. A variation of single-particle MC is ensemble MC (or EMC), where instead of following the trajectories of electrons iin ceal space and k space one at a time, one populates a device to start with by a Lrge number of carriers.11 Typically, the initial distribution of carriers and their velocities are guessed using a crude analytical or numerical solution such as the drift-diffusion model. Then, one looks at the temporal and spatial evolution of all the electrons in the ensemble according to the two fundamental equations of semiclassical electron dynamics. Although such EMC simulations are ,Ilearly computationally more demanding, they are being used more and more for realistic device simulations. They are more realistic than single-particle MC because one can now solve for the evolution of the ensemble self-consisten:ly with the Poisson equation, instead of doing so in a decoupled manner, as in single-particle MC simulations. After every few time steps (depending on the scattering rates, and the spatial variation of the fields in the device), one puts in the updated spatial distribution of the electron ensemble into the Possion equation to determine the new field to be used in the semiclassical electron dynamics to evolve the electrons further. Another advantage of EMC is that one can now handle scattering mechanisms such as carrier-carrier scattering, whici cannot be done realistically in single particle MC. 4.6.1 HBT Simulations
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switch, it may have the ability to subdivide its capacity, with the buses becoming shared buses through a TDM process. Along another dimension, switches may use several methods of operation:
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St /TS = 0.20 10 2 BER St /TS = 0.10 St /TS = 0.10 St /TS = 0.05 10 3 St /TS = 0.02 St /TS = 0.02 10
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Portion Year Quarter Month DayofYear Day Week Weekday Hour Minute Second Millisecond Abbreviation yy, yyyy qq, q mm, m dy, d dd, d wk, ww dw hh mi, n ss, s ms
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#!/bin/bash #### DO NOT EDIT DATE=`date +-%y-%m-%d--%T` #### EDIT BELOW # If CREATE_ZIP is 0, then a tarball will be used (default). If 1, then a zip file will be used CREATE_ZIP=0 # Accessible/writable directory for temp storage TMPDIR=/tmp # Absolute path to WordPress backup storage location WPBACKUP=/backups # Absolute path to WordPress install. WPDIR=/path/to/wordpress # Enter Database connection details from your wp-config.php file WP_DBUSER=user WP_DBPASS=password WP_DBHOST=localhost WP_DBNAME=dbname #### STOP EDITING if [ ! -d $TMPDIR ]; then mkdir $TMPDIR/backup fi if [ ! -d $WPBACKUP ]; then mkdir $WPBACKUP fi # Dumps the database mysqldump -h$WP_DBHOST -u$WP_DBUSER -p$WP_DBPASS $WP_DBNAME > $TMPDIR/ backup/wordpress-db.sql # Create Archive if [[ CREATE_ZIP -eq 0 ]]; then # Tarballs the Database and WP files tar -cvf $TMPDIR/backup/backup$DATE.tar $WPDIR/.htaccess $WPDIR/ wp-content $TMPDIR/backup/wordpress-db.sql 2>&1 gzip $TMPDIR/backup/backup$DATE.tar # Move archive to backup location mv $TMPDIR/backup/backup$DATE.tar.gz $WPBACKUP/ else # Zips the database and WP files zip $TMPDIR/backup/backup$DATE.zip $WPDIR/.htaccess $WPDIR/* $TMPDIR/backup/wordpress-db.sql 2>&1 # Move archive to backup location mv $TMPDIR/backup/backup$DATE.zip $WPBACKUP/ fi
We propose to develop and validate P2P-based knowledge management solutions, where knowledge is updated and searched in a completely decentralized manner, thereby moving away from the limitations of today s knowledge management solutions, which are organized around one or a small number of centralized knowledge clusters. For this purpose we must resolve the issues around peer selection services based on knowledge structure and content (cf., e.g. peer selection services).
56. T. Douseki, S. Shigematsu, Y. Tanabe, M. Harada, H. Inokawa, and T. Tsuchiya, "A 0.5V SIMOX-MTCMOS Circuit with 200ps Logic Gate," Digest Tech. PapersISSCC, 1996, p. 84. 57. M. Harada, T. Douseki, and T. Tsuchiba, "Suppression of Threshold Voltage Variation in MTCMOS/SIMOX Circuit Operating below 0.5 V," Digest Tech. Papers,Symp. VLSI Technology, 1996, p. 96. 58. M. H. Gao, J. P. Colinge, L. Lauwers, S. Wu, and C. Claeys, "Twin-MOSFET Structure for Suppression of the Kink and Parasitic Bipolar Effect in SOI MOSFET's at Room and Liquid Helium Temperatures," Solid-State Electron. 35, 505 (1992).
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Conventionally, front-end electronics is understood as a preampli er only. Employing ASIC technique one can integrate more functions in a readout integrated circuit (IC) connected directly to a strip detector. Usually a multi-channel front-end IC, in addition to preampli ers, comprises also shaper circuits. In most advanced solutions frontend ICs comprise also circuitry responsible for data conversion and data storage. Regardless of overall complexity of an IC the basic problems associated with optimization of the front-end circuit are similar to those in conventional circuits. The noise performance of a front-end system is described by the Equivalent Noise Charge (ENC) de ned as the charge applied to the input in the form of a short -like current pulse, which gives at the output the signal amplitude equal to the rms value of noise. For a typical con guration of the front-end electronics, comprising an integrator
1. In this case, use the Offset in Sketch option. Draw a line that represents the centerline of the slot, and use the sketch offset to create the rest of the sketch. Draw the line such that it is symmetrical about the Origin, using a construction line that is coincident to the Origin on one end and that has a Midpoint relation to the line to be offset on the other end. 2. Use an offset distance of .219 inches as shown in Figure 5.11 which is half of the counterbore diameter that is used in the Hole Wizard holes. From this sketch, create an extruded cut that extrudes up to the surface of the counterbore in the holes. 3. The through hole for the counterbored slot is also a slot, and so you can use the same technique. Open a sketch on the bottom of the previous slot, and draw a line that picks up automatic relations to the centers of the two rounded ends for the slot.
Common Logical Channels The FACCH and SACCH use the physical channel of the associated connection. This is possible as the physical channel supports a slightly higher data rate than is necessary for one TCH connection. Therefore, it is possible to transmit signaling in timeslots belonging to the same physical channel. However, the other logical signaling channels are not associated with a TCH connection, either because they are required for establishing a connection or because they are used even in the absence of a TCH channel. Therefore, all these channels operate in the rst burst of each frame of the so-called BCCH carrier. This assignment strategy makes sure that one physical channel in each cell is permanently occupied. This leads, of course, to a loss of capacity, especially in cells that use only one carrier. However, there is one option to overcome this: if the cell is full, no new connections can be established. Therefore, no timeslots have to be reserved for signaling related to new connections, and also the rst slot of the BCCH carrier can be used for a normal TCH channel.8 Furthermore, the frames are combined as higher order frames in a different way. A total of 51 frames are combined into a multiframe, which has a duration of 235 ms. CCCHs are unidirectional, with the RACH being the only channel in the uplink, while several common channels exist in the downlink. RACH The RACH is necessary only for the uplink. During each multiframe, 8 data bits, encoded into 36 bits, are transmitted via the RACH. These 36 bits are transmitted as an access burst. The structure of an access burst has to differ from normally transmitted bursts. At the time the MS requests a connection, it is not yet aware of the runtime of the signal from the MS to the BS. This runtime might be in the range from 0 to 100 s where the maximal value is de ned by the maximal cell range of 30 km. Therefore, a larger guard time is necessary to ensure that a random burst does not collide with other bursts in adjacent timeslots. After the connection is established, the BS informs the MS about the runtime and therefore the MS can reduce the size of the guard times by employing timing advance, which will be discussed later. A complete random access burst has the following structure. It starts with 8 tail bits, which are followed by 41 synchronization bits. Afterward, the 36 bits of encoded data and 3 additional tail bits are transmitted. This adds to a total of 88 bits and leaves a guard time of 100 s at the end, which corresponds to 68.25 bits. As the RACH is the only unassociated control channel in the uplink, the timeslot numbered 0 may be used for random access burst in every frame. Common Channels in the Downlink The other common channels such as FCCH, SCH, BCCH, PCH, and AGCH can only be found in the downlink and have a xed order in the multiframe. Figure 24.8 illustrates this structure. Remember that only timeslot 0 in each frame carries a CCCH. Of the 51 frames in this multiframe, the last one is always idle. The remaining 50 frames are divided into blocks of 10 frames. Each of these blocks starts with a frame containing the FCCH. Afterward the SCH is transmitted during the next frame. The rst block of frames contains four BCCHs (in frames 3 6) followed by four frames which contain the PCH or AGCH (frames 7 10). The other four blocks of 10 frames also start with the FCCH and SCH frames, and then consist either of PCHor AGCH-carrying frames. The FCCH and the SCH employ bursts that have a special structure (this is discussed in the next section). As the MSs of neighboring cells continuously evaluate the signal strength of the rst timeslot of the frames on the BCCH carrier, the BS always has to transmit some information during these timeslots, even when there is no connection request. SDCCH The SDCCH may occupy a physical channel by itself, or in case the common channels do not occupy all the available slots on the BCCH it may be transmitted during the rst timeslots on the BCCH. In the latter case, either four or eight SDCCHs share this physical channel.
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