STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
Section 5.5. In the following two sections, measurements of the HOM frequency, QL and polarization, which are used to characterize the HOMs, are discussed in detail. 4.6.1 RF Measurements of the Zone 3 Cryomodule In February 2004, the zone 3 cryomodule was moved into the FEL vault for installation and commissioning. Initially, the cryomodule sat parallel to its final destination on the beamline so it could be commissioned in parallel with standard FEL operations. When the cryomodule was cooled to 2 K, and before the final waveguides were installed, measurements of the HOM parameters were performed. For each of the eight cavities, the frequencies and loaded quality factors of the TM010 fundamental passband and TE111 and TM110 dipole mode passbands were measured. The details of the setup for measuring the HOM parameters are shown pictorially in Fig 4.5. A network analyzer (NWA) was used to manually measure the S21 scattering transmission parameter (see Appendix B). This involves using port 1 of the NWA to excite the cavity through the fundamental power coupler. The FPC is connected to a WR-650 waveguide-to-coaxial adapter (frequently called a top hat). The top hat is used to provide the proper impedance match from the waveguide to a 50 Ω coaxial cable. Port 2 of the NWA is connected to the cavity’s HOM1 port while the field probe and HOM2 ports are terminated in 50 Ω loads. This completes the S21 measurement. A manual search and measurement of each HOM is necessary. The frequency of individual HOMs are measured with an accuracy of up to 1 kHz. The loaded quality factor of each mode is found from the center frequency divided by the bandwidth between the −3 dB points. A typical HOM resonance curve with markers at the −3 dB points is shown in Fig. 4.6. In some instances, the interference of neighboring 99
FIG. 4.5: Setup for measuring cavity HOMs of zone 3 in the FEL vault. The upper left inset shows the top hat and the lower right inset shows the connections to HOM ports. 100
- Page 67 and 68: primary source of error is measurin
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- Page 71 and 72: TABLE 2.3: Comparison of Twiss para
- Page 73 and 74: the results of the fits. The vertic
- Page 75 and 76: FIG. 2.18: Schematic illustrating t
- Page 77 and 78: FIG. 2.19: The GASK signal measured
- Page 79 and 80: FIG. 2.20: The measured normalized
- Page 81 and 82: CHAPTER 3 The Jefferson Laboratory
- Page 83 and 84: FIG. 3.1: Schematic of the 10 kW FE
- Page 85 and 86: FIG. 3.2: Layout of the DC photocat
- Page 87 and 88: accelerating gradient at the front
- Page 89 and 90: eason for making the endloops achro
- Page 91 and 92: FIG. 3.7: Illustration of path leng
- Page 93 and 94: 3.5 Longitudinal Dynamics This sect
- Page 95 and 96: FIG. 3.9: The effect of a thin focu
- Page 97 and 98: Under the constraint that each orde
- Page 99 and 100: form of beam breakup not only occur
- Page 101 and 102: 4.1 The Pillbox Cavity Although the
- Page 103 and 104: FIG. 4.2: Electric field (red) and
- Page 105 and 106: where the full 4×4 transfer matrix
- Page 107 and 108: The threshold is inversely proporti
- Page 109 and 110: 4.3 BBU Simulation Codes: Particle
- Page 111 and 112: 6. The second pass beam bunch then
- Page 113 and 114: which excites it. The BBU instabili
- Page 115 and 116: Equation (4.41) is a dispersion rel
- Page 117: FIG. 4.4: Output from MATBBU showin
- Page 121 and 122: Consequently, depending on the exte
- Page 123 and 124: The projection of the beam displace
- Page 125 and 126: TABLE 4.1: Experimental measurement
- Page 127 and 128: FIG. 4.10: A plot showing the effec
- Page 129 and 130: these cryomodules. Modes from these
- Page 131 and 132: CHAPTER 5 Experimental Measurements
- Page 133 and 134: threshold current - preferably with
- Page 135 and 136: occurred at approximately 2 mA of a
- Page 137 and 138: FIG. 5.5: FFT of a pure 2106.007 MH
- Page 139 and 140: FIG. 5.6: Illustration to show the
- Page 141 and 142: 5.4 Measuring the Threshold Current
- Page 143 and 144: for the HOM-beam system and is deri
- Page 145 and 146: FIG. 5.10: Schematic of the experim
- Page 147 and 148: FIG. 5.12: A plot of 1/Qeff versus
- Page 149 and 150: measured HOMs in zone 3, a BTF meas
- Page 151 and 152: FIG. 5.16: HOM voltage measured fro
- Page 153 and 154: FIG. 5.18: A plot of the three valu
- Page 155 and 156: the beam’s response in regions wh
- Page 157 and 158: CHAPTER 6 BBU Suppression: Beam Opt
- Page 159 and 160: FIG. 6.1: Schematic of a FODO cell
- Page 161 and 162: plane [85]. Equations (6.7) and (6.
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Section 5.5. In the following two sections, measurements of the HOM frequency, QL<br />
and polarization, which are used to characterize the HOMs, are discussed in detail.<br />
4.6.1 RF Measurements of the Zone 3 Cryomodule<br />
In February 2004, the zone 3 cryomodule was moved into the FEL vault for<br />
installation and commissioning. Initially, the cryomodule sat parallel to its final<br />
destination on the beamline so it could be commissioned in parallel with standard<br />
FEL operations. When the cryomodule was cooled to 2 K, and before the final<br />
waveguides were installed, measurements of the HOM parameters were performed.<br />
For each of the eight cavities, the frequencies and loaded quality factors of the TM010<br />
fundamental passband and TE111 and TM110 dipole mode passbands were measured.<br />
The details of the setup for measuring the HOM parameters are shown pictorially<br />
in Fig 4.5.<br />
A network analyzer (NWA) was used to manually measure the S21 scattering<br />
transmission parameter (see Appendix B). This involves using port 1 of the NWA<br />
to excite the cavity through the fundamental power coupler. The FPC is connected<br />
to a WR-650 waveguide-to-coaxial adapter (frequently called a top hat). The top<br />
hat is used to provide the proper impedance match from the waveguide to a 50 Ω<br />
coaxial cable. Port 2 of the NWA is connected to the cavity’s HOM1 port while the<br />
field probe and HOM2 ports are terminated in 50 Ω loads. This completes the S21<br />
measurement.<br />
A manual search and measurement of each HOM is necessary. The frequency of<br />
individual HOMs are measured with an accuracy of up to 1 kHz. The loaded quality<br />
factor of each mode is found from the center frequency divided by the bandwidth<br />
between the −3 dB points. A typical HOM resonance curve with markers at the<br />
−3 dB points is shown in Fig. 4.6. In some instances, the interference of neighboring<br />
99