Home > Research > Publications & Outputs > Components for the testing of a co-harmonic gyr...
View graph of relations

Components for the testing of a co-harmonic gyrotron cavity

Research output: Contribution to conference - Without ISBN/ISSN Conference paperpeer-review

Published

Standard

Components for the testing of a co-harmonic gyrotron cavity. / Constable, D. A.; Ronald, Kevin; He, Wenlong et al.
2010. Paper presented at National Vacuum Electronics Conference (NVEC) 2010, Daresbury, United Kingdom.

Research output: Contribution to conference - Without ISBN/ISSN Conference paperpeer-review

Harvard

Constable, DA, Ronald, K, He, W, Fampris, XS, Phelps, ADR & Cross, AW 2010, 'Components for the testing of a co-harmonic gyrotron cavity', Paper presented at National Vacuum Electronics Conference (NVEC) 2010, Daresbury, United Kingdom, 14/07/10 - 15/07/10.

APA

Constable, D. A., Ronald, K., He, W., Fampris, X. S., Phelps, A. D. R., & Cross, A. W. (2010). Components for the testing of a co-harmonic gyrotron cavity. Paper presented at National Vacuum Electronics Conference (NVEC) 2010, Daresbury, United Kingdom.

Vancouver

Constable DA, Ronald K, He W, Fampris XS, Phelps ADR, Cross AW. Components for the testing of a co-harmonic gyrotron cavity. 2010. Paper presented at National Vacuum Electronics Conference (NVEC) 2010, Daresbury, United Kingdom.

Author

Constable, D. A. ; Ronald, Kevin ; He, Wenlong et al. / Components for the testing of a co-harmonic gyrotron cavity. Paper presented at National Vacuum Electronics Conference (NVEC) 2010, Daresbury, United Kingdom.

Bibtex

@conference{faa8edbbd74d4639be9bf545872a5b98,
title = "Components for the testing of a co-harmonic gyrotron cavity",
abstract = "A primary objective for the field of vacuum electronics is the development ofdevices capable of generating coherent, high power radiation within the sub-mmregime. The electron cyclotron maser instability offers an attractive method offulfilling such requirements, being a well established mechanism for obtainingcoherent, high power radiation within the mm-band. However, operation at highharmonics of the electron cyclotron frequency, ωc, proves challenging, given thesensitivity of parasitic modes to the large beam currents required.Previously, particle-in-cell simulations have been presented on thesimultaneous operation of a gyrotron cavity at the 2nd and 4th harmonics of theelectron cyclotron frequency[1]. Such a co-harmonic scheme is used to obtain high frequency radiation through the direct excitation of a low harmonic signal. By then trapping the low harmonic within the interaction region, through the use of a cut-off aperture, pure output of the high harmonic signal can be realised. However, the intended output radiation is dominated by a mode converted 2nd harmonic signal.Analysis of the setup suggests that such mode conversion occurs due to the cut-off aperture, and while the magnitude of the converted signal can be reduced, it cannot be eliminated entirely.As a result, the current focus is to confirm the presence of this modeconversion experimentally. To that end, the design and fabrication of severaladditional components has been required. A brief overview of these components will be given, along with some initial experimental results",
author = "Constable, {D. A.} and Kevin Ronald and Wenlong He and Fampris, {Xenofon S.} and Phelps, {Alan D. R.} and Cross, {Adrian W.}",
year = "2010",
month = jul,
day = "15",
language = "English",
note = "National Vacuum Electronics Conference (NVEC) 2010, NVEC ; Conference date: 14-07-2010 Through 15-07-2010",
url = "http://indico.hep.manchester.ac.uk/conferenceDisplay.py?ovw=True&confId=2288",

}

RIS

TY - CONF

T1 - Components for the testing of a co-harmonic gyrotron cavity

AU - Constable, D. A.

AU - Ronald, Kevin

AU - He, Wenlong

AU - Fampris, Xenofon S.

AU - Phelps, Alan D. R.

AU - Cross, Adrian W.

PY - 2010/7/15

Y1 - 2010/7/15

N2 - A primary objective for the field of vacuum electronics is the development ofdevices capable of generating coherent, high power radiation within the sub-mmregime. The electron cyclotron maser instability offers an attractive method offulfilling such requirements, being a well established mechanism for obtainingcoherent, high power radiation within the mm-band. However, operation at highharmonics of the electron cyclotron frequency, ωc, proves challenging, given thesensitivity of parasitic modes to the large beam currents required.Previously, particle-in-cell simulations have been presented on thesimultaneous operation of a gyrotron cavity at the 2nd and 4th harmonics of theelectron cyclotron frequency[1]. Such a co-harmonic scheme is used to obtain high frequency radiation through the direct excitation of a low harmonic signal. By then trapping the low harmonic within the interaction region, through the use of a cut-off aperture, pure output of the high harmonic signal can be realised. However, the intended output radiation is dominated by a mode converted 2nd harmonic signal.Analysis of the setup suggests that such mode conversion occurs due to the cut-off aperture, and while the magnitude of the converted signal can be reduced, it cannot be eliminated entirely.As a result, the current focus is to confirm the presence of this modeconversion experimentally. To that end, the design and fabrication of severaladditional components has been required. A brief overview of these components will be given, along with some initial experimental results

AB - A primary objective for the field of vacuum electronics is the development ofdevices capable of generating coherent, high power radiation within the sub-mmregime. The electron cyclotron maser instability offers an attractive method offulfilling such requirements, being a well established mechanism for obtainingcoherent, high power radiation within the mm-band. However, operation at highharmonics of the electron cyclotron frequency, ωc, proves challenging, given thesensitivity of parasitic modes to the large beam currents required.Previously, particle-in-cell simulations have been presented on thesimultaneous operation of a gyrotron cavity at the 2nd and 4th harmonics of theelectron cyclotron frequency[1]. Such a co-harmonic scheme is used to obtain high frequency radiation through the direct excitation of a low harmonic signal. By then trapping the low harmonic within the interaction region, through the use of a cut-off aperture, pure output of the high harmonic signal can be realised. However, the intended output radiation is dominated by a mode converted 2nd harmonic signal.Analysis of the setup suggests that such mode conversion occurs due to the cut-off aperture, and while the magnitude of the converted signal can be reduced, it cannot be eliminated entirely.As a result, the current focus is to confirm the presence of this modeconversion experimentally. To that end, the design and fabrication of severaladditional components has been required. A brief overview of these components will be given, along with some initial experimental results

M3 - Conference paper

T2 - National Vacuum Electronics Conference (NVEC) 2010

Y2 - 14 July 2010 through 15 July 2010

ER -