Engineering topics
Farkas, Z.
Publications and source records attributed to Farkas, Z..
Superconducting Cavities and Modulated RF
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Recent Developments in the Microwave BEAM Position Monitors at SLAC
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Precision Energy Measurement Technique
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Some Aspects of Superconducting Accelerator Design
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Constant Amplitude RF to Periodic Pulses Converter
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Particle Acceleration with TE(011) Cavity
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The Roles of Frequency and Aperture in Linac Accelerator Design
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DYNAMICS OF AN ELECTRON IN AN RF GAP
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RF Pulse Compression Experiment at SLAC
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RADIOFREQUENCY PULSE COMPRESSION EXPERIMENTS AT SLAC
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SLED-II: A New Method of RF Pulse Compression
In the SLED 1 method of RF pulse compression, two high Q resonators store energy from an RF source for a relatively long time interval (typically 3 to 5 J.1sec). Triggered by a reversal in RF phase, this stored energy is then released during a much shorter interval equal to the filling time of the accelerating structure. A peak power gain on the order of three and a compression efficiency on the order of 60% are typically attained. The shape of the output pulse is, however, a sharply decaying expo- nential. In SLED-II the two cavities are replaced by two lengths of resonant line, forming a Resonant Line SLED (RELS) and resulting in a flat output pulse. Therefore, RELS stages can be cascaded to give a greater peak power gain. Using two stages, a peak power gain greater than ten can be achieved with a reasonable compression efficiency. Unlike the BEC,2 the RELS compression fac- tor per stage is not limited to two, albeit at the expense of intrinsic efficiency. Like the BEC, it uses long lines rather than short cavities.
Two-klystron Binary Pulse Compression at SLAC
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