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1 kbps data service on a DL DPDCH in the FDD mode We will then use the same parameters as employed in the first example and show the multirate services can bemapped to the corresponding UL DPCH how in TDD mode 132413 Mapping Several Multirate Services to the UL Physical Channels in FDD Mode [SS] In this example, we assume that a 41 kbps speechservice and a 64 kbps video service are to be transmitted simultaneously on UL The parametersused for this example the are shown in Table 17 As illustrated in Figure 132, a 16-bit CRC checksum is first attached to each transport block of DCH#l, that is, #la, ..,#ld, as wellas the transport block of DCH#2 for the purpose of error detection.

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Note: You also can preview the animation by running the entire slide show. See 13 to learn how to run a slide show.

Figure 10-8: Results from ReadToEnd method Figure 10-9 displays the text file that the StreamReader was reading from.

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the phonons, one invokes the acoustic or optic phonon deformation potential theory of Bardeen and Shockley The essence of the theory is that the phonon modes cause a local deformation of the lattice constant Since the bandgap is a function of the interatomic spacing, there will thus be a "local" modulation of the conduction- and valence-band edges in a random fashion as the phonons propagate through the crystal, leading to a perturbing (scattering) Hamiltonian In compound semiconductors, there can be additional scattering terms due the coulombic fields that are set up This leads to polar optic-phonon scattering (for the optic modes) or piezoelectric scattering (for the acoustic modes) We wtll not treat these here because they are not relevant for Si-based ULSI devices.

As a result, the number of bits in the transport block of Service 1 and Service 2 is increased to 640 + 16 = 656 bits and 164 + 16 = 180 bits,.

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RRC signaling messages are listed in Table 13.4-4. UTRAN standards specify message formats in the ASN.1 notation (Section 16.2) [46], which makes it impractical to show their bit maps in concise form. The reader interested in the detailed formats is referred to [45]. As an example of message contents, Table 13.4-5 shows the most signi cant information elements in the uplink Direct Transfer message. The CN Domain Identity IE has two values: Circuit-Switched Domain and Packet-Switched Domain. The NAS message IE contains the message to/from the core network (the Non-Access Stratum). 13.4.7 UTRAN Call Sequences

One calculates the matrix element of this Hamiltonian, now between a final coupled electron-phonon state and an initial electron-phonon state, instead of just between electron states, as in the previous calculations This is because electronphonon interactions will not only change the electron wavevector and energy, but will also change the phonon occupancy of the phonon bath in the crystal If the scattering involves phonon absorption, the final state will have one fewer phonon, while phonon emission will lead to an increase of the phonon occupancy number The main difference between the deformation potentials for the acoustic and optic branches is that in the former, since adjacent atoms move in phase, the local deformation of the lattice is dependent on the divergence of the atomic displacement vectors For the optic branch, where the nearest-neighbor atoms move against each other, out of phase, the local deformation depends on the displacement itself.

Block # 12

For the acoustic mode, using the Taylor series, we write the band-edge shifts with lattice deformation as AE, = Ec(a) - E, 1c + 6a) = \ da or in three dimensions AE, ox.

The white serial noise that is due to thermal uctuations in the transistor channel scales with 1/ , the 1/f low frequency noise due to trapping of charge carriers in the vicinity of the channel is independent of shaping and the parallel noise due to detector and gate leakage current as well as the feedback resistor contribution grows with . The leakage current has its physical origin in the thermal generation of electron hole pairs in the semiconductor through energy levels in the forbidden band gap. Those levels may arise from (mainly) metal contamination in the silicon or imperfections in the silicon lattice. In the case of mid-band-gap traps, the leakage current attenuates approximately a factor of two every 7 K in temperature reduction. In the case of the low frequency, or 1/f noise, electrically active traps capture and release the charge carriers in the transistor channel and therefore give rise to

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