1987
DOI: 10.1016/0168-9002(87)90125-2
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Equilibrium phase instability in the double RF system for Landau damping

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Cited by 17 publications
(9 citation statements)
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“…The dipole mode zero-frequency instability criterion may also be obtained as the condition under which the rf generator voltages do not provide a restoring force for slow rigid bunch motions in which the wake fields move with the bunch [19]; the instability is known accordingly as the equilibrium phase instability [3]. When zero-frequency instability is avoided, the Robinson damping rate is given by Equations (13)- (16) may be obtained directly for the dipole mode by assuming a rigid bunch motion in the synchrotron potential produced by two rf cavities [5].…”
Section: Single-mode Robinson Instability Formulasmentioning
confidence: 99%
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“…The dipole mode zero-frequency instability criterion may also be obtained as the condition under which the rf generator voltages do not provide a restoring force for slow rigid bunch motions in which the wake fields move with the bunch [19]; the instability is known accordingly as the equilibrium phase instability [3]. When zero-frequency instability is avoided, the Robinson damping rate is given by Equations (13)- (16) may be obtained directly for the dipole mode by assuming a rigid bunch motion in the synchrotron potential produced by two rf cavities [5].…”
Section: Single-mode Robinson Instability Formulasmentioning
confidence: 99%
“…A radio frequency cavity with resonant frequency near a harmonic of the fundamental rf cavity may increase Landau damping of synchrotron oscillations and lengthen the bunch, thereby suppressing coupled-bunch instabilities and increasing the Touschek lifetime [1][2][3][4][5][6][7][8][9]. A Landau cavity may be operated in passive mode, where its voltage is induced by the beam current, or active mode, where its voltage is maintained by an rf power supply and feedback.…”
Section: Introductionmentioning
confidence: 99%
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“…However, these references (and the many cited therein) are typically restricted to simple harmonic motion in all three planes; in particular, most theoretical approaches neglect the effects of Landau damping that arise when the longitudinal motion is nonlinear. While this approximation is valid for short bunches in single rf systems as is often the case, it does not describe multiple rf systems that are used to lengthen the bunch and increase Landau damping [5][6][7][8][9][10][11], and it fails for the extreme stretching and highly nonlinear (possibly quartic) longitudinal potentials planned for many ultralow emittance light sources (see, e.g., [12]).…”
Section: Introductionmentioning
confidence: 99%
“…Higher harmonic cavities, also known as Landau cavities, have been proposed and tested [1][2][3][4][5] as a means of introducing Landau damping for controlling beam instabilities and/or improving the beam lifetime due to large-angle intrabeam (Touschek) scattering. Touschek scattering is particularly important for storage rings such as the Advanced Light Source (ALS) because of the high density of electrons resulting from the small transverse beam size and the moderately low beam energy of 1.5 to 1.9 GeV.…”
Section: Introductionmentioning
confidence: 99%