STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
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the coupling of the HOM coupler is required. Such an undertaking is complicated by<br />
the fact that only simple analytic models have been used to estimate the magnitude<br />
of the steering and coupling effects. For instance, a formula for the magnitude of<br />
the dipole steering exists but assumes that each cavity operates with an accelerating<br />
gradient of 5 MV/m, which is not the case in reality [33]. Estimates of the magnitude<br />
of the coupling due to a single cavity have been made [31], however it neglects<br />
the effects of the betatron phase advance which can play an important role for an<br />
extended linac like in CEBAF [45].<br />
Extracting Twiss Parameters<br />
In addition to measuring the emittance, the Twiss parameters prior to the<br />
scanning quadrupole can be determined. With knowledge of the emittance and<br />
of the fitting coefficients (β1ɛg), (α1ɛg) and (γ1ɛg) the Twiss parameters are easily<br />
calculated and can be compared with the model optics. The linear optics code<br />
Optim was used to model the CEBAF-ER lattice. The results of the model optics<br />
and of the experimental measurements are displayed in Table 2.3. The agreement<br />
is very good, on the level of 5%, and further justifies the choice of data points used<br />
for fitting. The large errors associated with the extracted betas and alphas are the<br />
result of propagating the relatively large errors from the corresponding emittances.<br />
Because a model optics does not exist for the machine configured with 20 MeV<br />
injection energy, the extracted Twiss parameters could not be compared to the<br />
model.<br />
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