1994
DOI: 10.1109/27.338269
|View full text |Cite
|
Sign up to set email alerts
|

Electromagnetic properties of open and closed overmoded slow-wave resonators for interaction with relativistic electron beams

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3

Citation Types

1
16
0

Year Published

1999
1999
2018
2018

Publication Types

Select...
8
1
1

Relationship

0
10

Authors

Journals

citations
Cited by 68 publications
(17 citation statements)
references
References 16 publications
1
16
0
Order By: Relevance
“…The theory of perfectly periodic RF structures has been extensively developed over many years, motivated largely by the many practical applications of periodic structures such as filters, antennas, and slow wave circuits, [1] and [2]. Of course, the practical realization of a periodic structure is never perfect, due to fabrication tolerances and/or variations in material properties from cell to cell.…”
Section: Introductionmentioning
confidence: 99%
“…The theory of perfectly periodic RF structures has been extensively developed over many years, motivated largely by the many practical applications of periodic structures such as filters, antennas, and slow wave circuits, [1] and [2]. Of course, the practical realization of a periodic structure is never perfect, due to fabrication tolerances and/or variations in material properties from cell to cell.…”
Section: Introductionmentioning
confidence: 99%
“…Finally, to shorten the interaction region the PASOTRON slow-wave structures are usually characterized by significant end reflections which cause transformation of a continuous ͑within the passband͒ spectrum of a wellmatched periodic slow-wave structure ͑SWS͒ into a discrete spectrum of standing modes with the same transverse structure but different numbers of axial variations. 6,7 The theory of relativistic BWOs with end reflections was developed in Ref. 6.…”
Section: Introductionmentioning
confidence: 99%
“…In the Pasotron, this depends on the amount of plasma generated by the beam that is required for sufficient beam propagation through the SWS with little or no applied magnetic field, 11 in order to support the oscillation. For trace ͑a͒ shown in Fig.…”
mentioning
confidence: 99%