Radio Frequency Quadrupole - CERN Accelerator School

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Why is the RFQ so efficient in �� Discrete bunching bunching a beam �� Vs adiabatic bunching : movie 32
Why is the RFQ so efficient in �� Discrete bunching bunching a beam �� Vs adiabatic bunching : movie 33
Page 1 and 2: Radio Frequency Quadrupole Alessand
Page 3 and 4: Contents �� Motivation and hist
Page 5 and 6: RFQ represented the “missing miss
Page 7 and 8: wave equation -recap recap �� M
Page 9 and 10: TE modes dipole mode quadrupole mod
Page 11 and 12: Radio Frequency Quadrupole cavity l
Page 13 and 14: vane four vane-structure vane struc
Page 15 and 16: + - transverse field in an RFQ - +
Page 17 and 18: acceleration in RFQ longitudinal mo
Page 19 and 20: important parameters of the RFQ B
Page 21 and 22: Beam dynamics design (very first ap
Page 23 and 24: Transverse plane-focusing plane foc
Page 25 and 26: Longitudinal plane-acceleration pla
Page 27 and 28: High intensity vs. low intensity Em
Page 29 and 30: modulation 2 1.8 1.6 1.4 1.2 1 0.8
Page 31: RFQ vs. DTL DTL can't accept low ve
Page 35 and 36: RFQ-summary RFQ summary �� The
Page 37 and 38: Further reading �� T.P.WANGLER,

Radio Frequency Quadrupole - CERN Accelerator School

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