The magnicon — An advanced version of the gyrocon

Karliner, Marek; Kozyrev, E.V.; Makarov, I. T.; Nezhevenko, O.A.; Ostreiko, G. N.; Persov, B.Z.; Serdobintsev, G. V.

doi:10.1016/0168-9002(88)90122-2

Cited by 66 publications

(20 citation statements)

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“…This first magnicon delivered 2.6 MW at 915 MHz with an efficiency of 85% [43]. The beam voltage and current for this experiment were 300 keV and 12 A, respectively, and the RF pulse length was 30 pus.…”

Section: Magniconsmentioning

confidence: 99%

RF sources for linear colliders

Danly¹

1995

AIP Conference Proceedings

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Section: Magniconsmentioning

confidence: 99%

RF sources for linear colliders

Danly¹

1995

AIP Conference Proceedings

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“…Different versions of magnicons have being built from the decimeter to the millimeter wavelength domains, operating in the first, second, and third harmonic modes. The first magnicon was built and tested in 1985 in Novosibirsk [3]. A power of 2.6 MW was obtained at 915 MHz with a pulse length of 30 µsec and electronic efficiency of 85%.…”

Section: B Technical Approachmentioning

confidence: 99%

120 MW, 800 MHz Magnicon for a Future Muon Collider

Hirshfield¹

2005

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“…The model includes beam loading effects, and allows analysis of tuning, tolerance requirements and beam loading. It was found that the most flexible and stable scheme of the structure excitation is the two-coupler scheme [11], where the input couplers excite independently the two orthogonal standing waves that comprise the resulting traveling wave. Multipactoring performance for the SC traveling wave accelerating (STWA) structure has been studied.…”

Section: We Define the Flatness Parameter As Flatness= (Max(e S ) -)/)mentioning

confidence: 99%

Conceptual design of an L-band recirculating superconducting traveling wave accelerating structure for ILC

Avrakhov

Kanareykin

Liu

et al. 2007

2007 IEEE Particle Accelerator Conference (PAC)

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With this paper, we propose the conceptual design of a traveling wave accelerating structure for a superconducting accelerator. The overall goal is to study a traveling wave (TW) superconducting (SC) accelerating structure for ILC that allows an increased accelerating gradient and, therefore reduction of the length of the collider. The conceptual studies were performed in order to optimize the acceleration structure design by minimizing the surface fields inside the cavity of the structure, to make the design compatible with existing technology, and to determine the maximum achievable gain in the accelerating gradient.The proposed solution considers RF feedback system redirecting the accelerating wave that passed through the superconducting traveling wave acceleration (STWA) section back to the input of the accelerating structure. The STWA structure has more cells per unit length than a TESLA structure but provides an accelerating gradient higher than a TESLA structure, consequently reducing the cost. In this paper, the STWA cell shape optimization, coupler cell design and feedback waveguide solution are considered. We also discuss the field flatness in the superconducting TW structure, the HOM modes and multipactor performance have been studied as well. The proposed TW structure design gives an overall 46% gain over the SW ILC structure if the 10 m long TW structure is employed.

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The magnicon — An advanced version of the gyrocon

Cited by 66 publications

References 1 publication

RF sources for linear colliders

RF sources for linear colliders

120 MW, 800 MHz Magnicon for a Future Muon Collider

Conceptual design of an L-band recirculating superconducting traveling wave accelerating structure for ILC

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