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(A 1.12)

(6.17)

locking scheme where conventional feedback from a diffraction grating is used. This does indeed suggest that the limited tuning range has to do with the injection locking process and not the properties of the phase conjugator. For a xed grating tilt and for a drive current of 2ith the FWHM bandwidth of the singlemode spectrum is measured to be less than 0.03 nm. By recording the frequencyresolved near- eld pattern with a setup similar to the one in Ref. 68, it is veri ed that the array only operates in one array mode. As the drive current is increased to 3ith, however, additional array modes start to oscillate and increase the bandwidth to 0.1 nm.

Table 30-3 IP Address and Subnet Mask = Network Address SUBNET MASK 1111 1111 1111 1111 1111 1111 1111 0000 255.255.255.240 NETWORK ADDRESS (BOOLEAN AND) 1101 0010 0000 1100 1101 1000 0101 0000 210.12.216.80

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Circular proton accelerators may require a significant frequency variation during the acceleration process. For instance, in the Fermilab booster synchrotron, the kinetic energy of protons is increased from 200 MeV to 8 GeV. The speed of the protons and hence the frequency of the accelerating system increases by a factor of 1.76 during this process. Suppose that our simple pillbox cavity were filled with a material of relative permeability K , = p / p o . Setting aside for the moment the problem of getting the particle beam through this device, the resonant frequency of the cavity will have been This can be easily seen by noting that reduced by a factor of 1/ Equation 2.4 will now contain a factor of K , on the right hand side. Now we need a mechanism for varying K , through the acceleration cycle. Figure 2.9 shows one approach to providing tunability while retaining the material-free passage for the beam.

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