Progress at SLAC on high-power rf pulse compression [electronic resource]

Rf pulse compression is a technique for augmenting the peak power output of a klystron (typically 50--100 MW) to obtain the high peak power required to drive a linear collider at a high accelerating gradient (typically 200 MW/m is required for a gradient of 100 MV/m). The SLED pulse compression syst...

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Bibliographic Details
Online Access: Online Access
Corporate Author: Stanford Linear Accelerator Center (Researcher)
Format: Government Document Electronic eBook
Language:English
Published: Washington, D.C. : Oak Ridge, Tenn. : United States. Dept. of Defense ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy, 1992.
Subjects:

MARC

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245 0 0 |a Progress at SLAC on high-power rf pulse compression  |h [electronic resource] 
260 |a Washington, D.C. :  |b United States. Dept. of Defense ;  |a Oak Ridge, Tenn. :  |b distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,  |c 1992. 
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500 |a Published through the Information Bridge: DOE Scientific and Technical Information. 
500 |a 06/01/1992. 
500 |a "slac-pub-5866" 
500 |a "DE93009730" 
500 |a Wilson, P.B.; Ruth, R.D.; Kroll, N.M. California Univ., San Diego; Farkas, Z.D.; Lavine, T.L.; Menegat, A.; Nantista, C. 
520 3 |a Rf pulse compression is a technique for augmenting the peak power output of a klystron (typically 50--100 MW) to obtain the high peak power required to drive a linear collider at a high accelerating gradient (typically 200 MW/m is required for a gradient of 100 MV/m). The SLED pulse compression system, with a power gain of about 2.6, has been operational on the SLAC linac for more than a decade. Recently, a binary pulse-compression system with a power gain of about 5.2 has been tested up to an output power of 120 MW. Further high-power tests are in progress. Our current effort is focused on prototyping a so-called SLED-II pulse-compression system with a power gain of four. Over-moded TE[sub 01]-mode circular waveguide components, some with novel technical features, are used to reduce losses at the 11.4-GHz operating frequency. 
536 |b AC03-76SF00515. 
650 7 |a Accelerator Facilities.  |2 local. 
650 7 |a High-voltage Pulse Generators.  |2 local. 
650 7 |a Stanford Linear Collider.  |2 local. 
650 7 |a Electronic Equipment.  |2 local. 
650 7 |a Pulse Generators.  |2 local. 
650 7 |a Klystrons.  |2 local. 
650 7 |a Rf Systems.  |2 local. 
650 7 |a Microwave Tubes.  |2 local. 
650 7 |a Electron Tubes.  |2 local. 
650 7 |a Equipment.  |2 local. 
650 7 |a Microwave Equipment.  |2 local. 
650 7 |a Linear Accelerators.  |2 local. 
650 7 |a Function Generators.  |2 local. 
650 7 |a Accelerators.  |2 local. 
650 7 |a Waveguides.  |2 local. 
650 7 |a Particle Accelerators.  |2 edbsc. 
710 2 |a Stanford Linear Accelerator Center.  |4 res. 
710 1 |a United States.  |b Department of Defense.  |4 spn. 
710 1 |a United States.  |b Department of Energy.  |4 spn. 
710 1 |a United States.  |b Department of Energy.  |b Office of Scientific and Technical Information.  |4 dst. 
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