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Passive components for the testing of a co-harmonic gyrotron cavity

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Passive components for the testing of a co-harmonic gyrotron cavity. / Constable, D. A.; Fampris, X. S.; Ronald, K. et al.
2nd Annual Passive RF and Microwave Components Seminar. 5. ed. IEEE, 2011. p. 81-82 (IET Seminar Digest; Vol. 2011, No. 5).

Research output: Contribution in Book/Report/Proceedings - With ISBN/ISSN › Conference contribution/Paper › peer-review

Harvard

Constable, DA, Fampris, XS, Ronald, K, He, W, Whyte, CG & Robertson, CW 2011, Passive components for the testing of a co-harmonic gyrotron cavity. in 2nd Annual Passive RF and Microwave Components Seminar. 5 edn, IET Seminar Digest, no. 5, vol. 2011, IEEE, pp. 81-82, 2nd Annual Passive RF and Microwave Components Seminar, Glasgow, United Kingdom, 30/03/11. https://doi.org/10.1049/ic.2011.0205

APA

Constable, D. A., Fampris, X. S., Ronald, K., He, W., Whyte, C. G., & Robertson, C. W. (2011). Passive components for the testing of a co-harmonic gyrotron cavity. In 2nd Annual Passive RF and Microwave Components Seminar (5 ed., pp. 81-82). (IET Seminar Digest; Vol. 2011, No. 5). IEEE. https://doi.org/10.1049/ic.2011.0205

Vancouver

Constable DA, Fampris XS, Ronald K, He W, Whyte CG, Robertson CW. Passive components for the testing of a co-harmonic gyrotron cavity. In 2nd Annual Passive RF and Microwave Components Seminar. 5 ed. IEEE. 2011. p. 81-82. (IET Seminar Digest; 5). doi: 10.1049/ic.2011.0205

Author

Constable, D. A. ; Fampris, X. S. ; Ronald, K. et al. / Passive components for the testing of a co-harmonic gyrotron cavity. 2nd Annual Passive RF and Microwave Components Seminar. 5. ed. IEEE, 2011. pp. 81-82 (IET Seminar Digest; 5).

Bibtex

@inproceedings{67d2ed604bf8490e9d9d2a7bcf6a2e9e,
title = "Passive components for the testing of a co-harmonic gyrotron cavity",
abstract = "A key design process in the construction of a waveguide cavity or component is the so-called cold test stage. This involves measuring the response of the component to radiation, propagating with a specific electromagnetic mode and a certain frequency, or range of frequencies. However, for components that require testing with high order modes, such as resonant cavities used in high-power, or high-harmonic gyrotrons, it can be challenging to generate the necessary mode. A scheme for co-harmonic generation of radiation through the cyclotron resonance maser (CRM) instability has previously been proposed. Such a scheme involves the generation of two separate harmonics of the electron cyclotron frequency, specifically the 2 nd and 4 th harmonics, within the same geometry. The two electromagnetic modes stimulated are the TE 2.2 and TE 4.3. Unfortunately, the generation of these two modes for cold testing purposes is not a trivial matter.",
author = "Constable, {D. A.} and Fampris, {X. S.} and K. Ronald and W. He and Whyte, {C. G.} and Robertson, {C. W.}",
year = "2011",
month = dec,
day = "1",
doi = "10.1049/ic.2011.0205",
language = "English",
isbn = "9781849193221",
series = "IET Seminar Digest",
publisher = "IEEE",
number = "5",
pages = "81--82",
booktitle = "2nd Annual Passive RF and Microwave Components Seminar",
edition = "5",
note = "2nd Annual Passive RF and Microwave Components Seminar ; Conference date: 30-03-2011 Through 30-03-2011",

}

RIS

TY - GEN

T1 - Passive components for the testing of a co-harmonic gyrotron cavity

AU - Constable, D. A.

AU - Fampris, X. S.

AU - Ronald, K.

AU - He, W.

AU - Whyte, C. G.

AU - Robertson, C. W.

PY - 2011/12/1

Y1 - 2011/12/1

N2 - A key design process in the construction of a waveguide cavity or component is the so-called cold test stage. This involves measuring the response of the component to radiation, propagating with a specific electromagnetic mode and a certain frequency, or range of frequencies. However, for components that require testing with high order modes, such as resonant cavities used in high-power, or high-harmonic gyrotrons, it can be challenging to generate the necessary mode. A scheme for co-harmonic generation of radiation through the cyclotron resonance maser (CRM) instability has previously been proposed. Such a scheme involves the generation of two separate harmonics of the electron cyclotron frequency, specifically the 2 nd and 4 th harmonics, within the same geometry. The two electromagnetic modes stimulated are the TE 2.2 and TE 4.3. Unfortunately, the generation of these two modes for cold testing purposes is not a trivial matter.

AB - A key design process in the construction of a waveguide cavity or component is the so-called cold test stage. This involves measuring the response of the component to radiation, propagating with a specific electromagnetic mode and a certain frequency, or range of frequencies. However, for components that require testing with high order modes, such as resonant cavities used in high-power, or high-harmonic gyrotrons, it can be challenging to generate the necessary mode. A scheme for co-harmonic generation of radiation through the cyclotron resonance maser (CRM) instability has previously been proposed. Such a scheme involves the generation of two separate harmonics of the electron cyclotron frequency, specifically the 2 nd and 4 th harmonics, within the same geometry. The two electromagnetic modes stimulated are the TE 2.2 and TE 4.3. Unfortunately, the generation of these two modes for cold testing purposes is not a trivial matter.

U2 - 10.1049/ic.2011.0205

DO - 10.1049/ic.2011.0205

M3 - Conference contribution/Paper

AN - SCOPUS:84865719224

SN - 9781849193221

T3 - IET Seminar Digest

SP - 81

EP - 82

BT - 2nd Annual Passive RF and Microwave Components Seminar

PB - IEEE

T2 - 2nd Annual Passive RF and Microwave Components Seminar

Y2 - 30 March 2011 through 30 March 2011

ER -