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The damping ring kickers for the SLAC Linear Collider must provide 7 mrad kicks to 1.2 GeV beams with 60 nsec rise and fall times and fit in a 50 cm length around a 21 mm diameter ceramic beam pipe. This requires that they operate at up to 40 KV. The construction and operation of two types of quasi-coaxial ferrite magnet potted with RTV silicone rubber is discussed. Production yield has been improved by changes in RTV degassing, transfer, and cure. Operation lifetime is dominated by voltage, radiation. and thermal cycling. I. DESIGN CONSIDERATIONSThe SLAC Linear Collider (SLC) damping rings are small 1.2 GeV synchrotrons used to reduce the emittance of e+ and ebunches by radiation damping before they are accelerated in the main linac to 50 GeV and collided. The damping ring revolution time is only 120 nsec, and 2 bunches circulate in each ring. so the kicker rise and fall times must be less than 60 nsec. The injection and extraction straight sections'provide no damping so their length was minimized, thus a 7 mrad kick is required to clear the injection and extraction septa. The kickers are located where ring bends were omitted for dispersion suppression. The energy, angle, aperture, and length requirements imply a current of order 2000 A, and the energy, angle, aperture, and time requirements determine a voltage of order 30 KV.The kickers were intended to be terminated transmission lines with the beam in the gap of the ferrite flux return [ 1.21. Ferrite-free current strip kickers would require nearly twice the current of ferrite kickers. Transmission line structures give the optimum pulse response. The magnet pulse is provided by several RG-220 coaxial cables in parallel, and another set of cables carries the pulse to a matched terminating load. The kickers are in the air outside an alumina ceramic beam pipe with a Kovar inner coating (about 1 ohm/square) that prevents the ferrite from being heated by beam image currents, and keeps the ferrite from loading the beam. The ceramic is 50 cm long, 21 mm diameter with 3 mm walls, with a capacitive choke joint at one end to prevent the coating from forming a shorted turn in the magnet, while still allowing beam image *
The damping ring kickers for the SLAC Linear Collider must provide 7 mrad kicks to 1.2 GeV beams with 60 nsec rise and fall times and fit in a 50 cm length around a 21 mm diameter ceramic beam pipe. This requires that they operate at up to 40 KV. The construction and operation of two types of quasi-coaxial ferrite magnet potted with RTV silicone rubber is discussed. Production yield has been improved by changes in RTV degassing, transfer, and cure. Operation lifetime is dominated by voltage, radiation. and thermal cycling. I. DESIGN CONSIDERATIONSThe SLAC Linear Collider (SLC) damping rings are small 1.2 GeV synchrotrons used to reduce the emittance of e+ and ebunches by radiation damping before they are accelerated in the main linac to 50 GeV and collided. The damping ring revolution time is only 120 nsec, and 2 bunches circulate in each ring. so the kicker rise and fall times must be less than 60 nsec. The injection and extraction straight sections'provide no damping so their length was minimized, thus a 7 mrad kick is required to clear the injection and extraction septa. The kickers are located where ring bends were omitted for dispersion suppression. The energy, angle, aperture, and length requirements imply a current of order 2000 A, and the energy, angle, aperture, and time requirements determine a voltage of order 30 KV.The kickers were intended to be terminated transmission lines with the beam in the gap of the ferrite flux return [ 1.21. Ferrite-free current strip kickers would require nearly twice the current of ferrite kickers. Transmission line structures give the optimum pulse response. The magnet pulse is provided by several RG-220 coaxial cables in parallel, and another set of cables carries the pulse to a matched terminating load. The kickers are in the air outside an alumina ceramic beam pipe with a Kovar inner coating (about 1 ohm/square) that prevents the ferrite from being heated by beam image currents, and keeps the ferrite from loading the beam. The ceramic is 50 cm long, 21 mm diameter with 3 mm walls, with a capacitive choke joint at one end to prevent the coating from forming a shorted turn in the magnet, while still allowing beam image *
The damping ring kickers for the SLAC Linear Collider must meet extreme requirements on rise and fall time, flatness, time and amplitude jitter and drift, voltage, repetition rate, and reliability. After several generations of improvements to the pulsers, magnets, and controls, and evolution in the understanding of the requirements, the kicker systems are no longer a serious constraint on SLC performance. Implications for future linear colliders are discussed.
Abstract?he difficulties with damping ring kickers that prevented operation of the SLAC Linear Collider in full multiple bunch mode have been overcome by shaping the current pulse to compensate for imperfections in the magnets. The risetime was improved by a peaking capacitor, with a tunable inductor to provide a locally flat pulse. The pulse was flattened by an adjustable droop inductor. Fine adjustment was provided by -pulse forming line tuners driven by stepping motors. Further risetime improvement will be obtained by a saturating ferrite -pulse sh&pener.The SLAC. Linear Collider (SLC) e-damping ring kickers must inject and extract 2 bunches on a single pulse, one for collision and one for e+ production, to produce full collision rate, The two bunches are 60 nsec apart, and must receive the same kick to 10-3 or better. The pulser risetime is marginal, and in addition the multigap thyratrons required for high voltage and fast rise time produce a series of prepulses as ths gaps break down. Neither of two different magnet designs has produced a field pulse with the desired risetime and flatness for 2 e-bunch extraction [l]. These problems combined to prevent operation with 2 bunches in the e-damping ring, allowing only half of the linac pulses to be used for collisions, with the other half used for e+ production. A program to produce a better magnet was undertaken, but progress was expected to be slow because the magnet faces additional constraints from size, high voltage, and radiation damage 121. A parallel program was therefore undertaken to control the pulse shape. II. SHAPING WITH LUMPED COMPONENTSThe e-extraction kicker pulser [3] uses 2 thyratrons in an oil filled tank to switch charged cables at the anodes into output cables at the floating cathodes to the magnet and its terminating load. Each thyratron switches 2 parallel 50 ohm cables, and 4 cables are paralleled at the magnet. The first method of pulse shaping was to connect inductors ("droop *
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