1956
DOI: 10.1007/978-3-642-92682-2
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Mathematische Methoden in der Hochfrequenztechnik

Abstract: Das Buch ist aus dem Bedurfnis heraus entstanden, die bei theoretischen Problemen der Hochfrequenztechnik am haufigsten ben6tigten mathematischen Hilfsmittel und Beziehungen in einem Band zur Hand zu haben. Eine Vollstandigkeit in irgendeinem Sinne kann dabei nicht beansprucht werden. Fur die Stoffauswahl hatte der Verfasser den Vorzug, sich auf die Ratschlage von Herrn Prof. Dr. W. KLEEN und die Erfahrungen mehrerer Kollegen stutzen zu k6nnen; ihnen allen sei fur ihre Unterstutzung gedankt. Es erschien zweck-… Show more

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Cited by 29 publications
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“…Due to the relatively strong coupling, resulting in a low loaded Q of our cavities, the measured resonance frequency is shifted by −20 MHz with respect to the resonance frequency calculated by using the diameter and the height of the cavity. The actual microwave field in the cavity can be described by a superposition of various field modes TE npq that are excited with different amplitudes and phases [32]. The model describes the field in the cavity to consist of a dominant TE 011 mode with losses, and other contributing modes which have no losses.…”
Section: Cavity Phase Shiftmentioning
confidence: 99%
“…Due to the relatively strong coupling, resulting in a low loaded Q of our cavities, the measured resonance frequency is shifted by −20 MHz with respect to the resonance frequency calculated by using the diameter and the height of the cavity. The actual microwave field in the cavity can be described by a superposition of various field modes TE npq that are excited with different amplitudes and phases [32]. The model describes the field in the cavity to consist of a dominant TE 011 mode with losses, and other contributing modes which have no losses.…”
Section: Cavity Phase Shiftmentioning
confidence: 99%