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Quantum Error Correction and Fault-Tolerant QC The discovery of the threshold result in fault-tolerant QC provided the theoretical basis for considering truly scalable physical implementations of QC. The original threshold result showed that as long as the decoherence rate is below 10 6, arbitrarily long quantum computations may be carried out. The error model here is that each gate is subject to decoherence independently with probability . More recent improvements by Aharonov and Gottesman [483] put the threshold at 10 4, and Steane [484] shows that under mild assumptions the threshold is 10 3. These improvements make use of quantum teleportation to prepare ancilla states [546] as well as improved use of quantum error-correcting codes. On the other hand, the best upper bound on the threshold was recently established by Razborov [485], who showed that if the threshold is below 1 , unless BQP BQNC. For scalable QC to 2 be practical, it is essential to improve the threshold by at least another order of magnitude.

Similarly, at the output, the load-re ection coef cient for the DUT L is set by another tuner, after which the signal is fed to another power sensor In fact, the source/load-pull set-up replicates a power ampli er, where the signal source with the ampli er and the isolator act as a matched input large-signal source, the tuners act as adjustable matching networks, the bias Ts act as bias networks and the output power sensor acts as a matched output load; the directional coupler is inserted only for measurement purposes Provided that the attenuation and the impedances of the tuners are accurately known, input and output power at the DUT for the given loading conditions are evaluated from the power sensors; power gain and ef ciency are also immediately computed if the DC power from the power supply is evaluated.

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The tuners are therefore the centrepieces of the set-up; they must be reliable, repeatable and exible enough to ensure accurate data Passive tuners can be mechanical or electronic Mechanical tuners are made of a piece of rectangular waveguide with a longitudinal slot in which one or two slugs are inserted (see Figure 22) The position along the slot and the depth of insertion of the slug(s) in the slot control the phase and the amplitude of the re ection coef cient respectively In manual.

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This command uses cat to generate the output of the file document and then uses the pipe to stream that output into the sed command, which makes the substitution. The output of the sed command is then redirected into a file called document-updated. Voila! You have just updated your file, and it only took a few seconds.

Podcatcher Software for Pocket PCs Egress PocketRSS Aggregators BlogMatrix Sparks FeedDemon NewsGator Smart Phones Podcatcher Resources Summary 30 31 31 32 33 34 34 36 36 36.

The performance of the art history brush depends both on the tool options that you select from the Options bar and the source state specified in the History palette. For information on setting the source state, read The History palette section, earlier in this chapter. From the Options bar, shown in Figure 7-37, you can select a brush, a brush mode, and the opacity just as you do when using the paintbrush, covered in 5. You can also use the Brush Dynamics options to create tapering and fading strokes using either a mouse or a pressure-sensitive palette. Read about these options in 5 as well.

Figures 2.2, 2.3

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