STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
[94] B. Yunn, in Proceedings of the European Particle Accelerator Conference, Lucerne, Switzerland, 2004 (2004), pp. 2218–2220. [95] G. Krafft, Private communication (2006). [96] G. Krafft, Phys. Rev. ST Accel. Beams 7, 060704 (2004). [97] J. Byrd and F. Casper, Beam Measurements (World Scientific, 1999), ISBN 981-02-3881-9. 203
VITA Christopher D. Tennant Christopher Daniel Tennant was born June 25, 1979 in Sidney, NY. He grad- uated from Bainbridge-Guilford High School in Bainbridge, New York in June of 1997. He graduated summa cum laude with a Bachelor of Arts in physics and a minor in mathematics from Ithaca College in Ithaca, New York in May 2001. He received a Master of Science degree in physics from the College of William and Mary in Williamsburg, Virginia in December 2002. This dissertation was defended on October 26, 2006 at the College of William and Mary in Virginia. 204
- Page 171 and 172: ⎛ ⎞ ⎜ ⎝ 0 0 0 0 0 −1/K 0
- Page 173 and 174: FIG. 6.11: A plot of 1/Qeff versus
- Page 175 and 176: FIG. 6.12: Threshold current for no
- Page 177 and 178: FIG. 6.14: Threshold current utiliz
- Page 179 and 180: TABLE 6.1: Summary of the measured
- Page 181 and 182: CHAPTER 7 BBU Suppression: Feedback
- Page 183 and 184: FIG. 7.1: A schematic of the feedba
- Page 185 and 186: FIG. 7.4: A coaxial 3-stub tuner us
- Page 187 and 188: All of these considerations are con
- Page 189 and 190: FIG. 7.6: Generic layout for a feed
- Page 191 and 192: in Section 4.2.1, however, in the p
- Page 193 and 194: FIG. 7.7: The threshold current as
- Page 195 and 196: FIG. 7.8: Threshold current versus
- Page 197 and 198: FIG. 7.10: The threshold current as
- Page 199 and 200: CHAPTER 8 Conclusions The work pres
- Page 201 and 202: le were experimentally measured. Du
- Page 203 and 204: APPENDIX A The Pillbox Cavity Start
- Page 205 and 206: FIG. A.1: A pillbox cavity exhibiti
- Page 207 and 208: Ez(ρ, φ) = ψ(ρ, φ) = E0Jm(γρ
- Page 209 and 210: FIG. B.1: Relationship of the S-par
- Page 211 and 212: FIG. C.1: Impedance and frequency o
- Page 213 and 214: FIG. C.5: Impedance and frequency o
- Page 215 and 216: BIBLIOGRAPHY [1] M. Tigner, Nuovo C
- Page 217 and 218: [22] L. Merminga, in Proceedings of
- Page 219 and 220: [50] C. Hernandez-Garcia et al., in
- Page 221: [79] L. Merminga et al., in Proceed
[94] B. Yunn, in Proceedings of the European Particle Accelerator Conference,<br />
Lucerne, Switzerland, 2004 (2004), pp. 2218–2220.<br />
[95] G. Krafft, Private communication (2006).<br />
[96] G. Krafft, Phys. Rev. ST Accel. Beams 7, 060704 (2004).<br />
[97] J. Byrd and F. Casper, Beam Measurements (World Scientific, 1999), ISBN<br />
981-02-3881-9.<br />
203