Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity
In the last few years superconducting radio-frequency (rf) cavities made of high-purity (residual resistivity ratio>200) niobium achieved accelerating gradients close to the theoretical limits. An obstacle towards achieving reproducibly higher fields is represented by “anomalous” losses causing a...
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American Physical Society
2006-04-01
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Series: | Physical Review Special Topics. Accelerators and Beams |
Online Access: | http://doi.org/10.1103/PhysRevSTAB.9.042001 |
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doaj-c7081a27c6ed42bcbc5fb493218d51552020-11-25T01:27:36ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022006-04-019404200110.1103/PhysRevSTAB.9.042001Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavityGianluigi CiovatiPeter KneiselIn the last few years superconducting radio-frequency (rf) cavities made of high-purity (residual resistivity ratio>200) niobium achieved accelerating gradients close to the theoretical limits. An obstacle towards achieving reproducibly higher fields is represented by “anomalous” losses causing a sharp degradation of the cavity quality factor when the peak surface magnetic field (B_{p}) is above about 90 mT, in the absence of field emission. This effect, called “Q drop” has been measured in many laboratories with single- and multicell cavities mainly in the gigahertz range. In addition, a low-temperature (100–140 °C) “in situ” baking of the cavity was found to be beneficial in reducing the Q drop. In order to gain some understanding of the nature of these losses, a single-cell cavity has been tested in the TM_{010} and TE_{011} modes at 2 K. The feature of the TE_{011} mode is to have zero electric field on the cavity surface, so that electric field effects can be excluded as a source for the Q drop. This article will present some of the experimental results for different cavity treatments and will compare them with existing models.http://doi.org/10.1103/PhysRevSTAB.9.042001 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Gianluigi Ciovati Peter Kneisel |
spellingShingle |
Gianluigi Ciovati Peter Kneisel Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity Physical Review Special Topics. Accelerators and Beams |
author_facet |
Gianluigi Ciovati Peter Kneisel |
author_sort |
Gianluigi Ciovati |
title |
Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity |
title_short |
Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity |
title_full |
Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity |
title_fullStr |
Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity |
title_full_unstemmed |
Measurement of the high-field Q drop in the TM_{010} and TE_{011} modes in a niobium cavity |
title_sort |
measurement of the high-field q drop in the tm_{010} and te_{011} modes in a niobium cavity |
publisher |
American Physical Society |
series |
Physical Review Special Topics. Accelerators and Beams |
issn |
1098-4402 |
publishDate |
2006-04-01 |
description |
In the last few years superconducting radio-frequency (rf) cavities made of high-purity (residual resistivity ratio>200) niobium achieved accelerating gradients close to the theoretical limits. An obstacle towards achieving reproducibly higher fields is represented by “anomalous” losses causing a sharp degradation of the cavity quality factor when the peak surface magnetic field (B_{p}) is above about 90 mT, in the absence of field emission. This effect, called “Q drop” has been measured in many laboratories with single- and multicell cavities mainly in the gigahertz range. In addition, a low-temperature (100–140 °C) “in situ” baking of the cavity was found to be beneficial in reducing the Q drop. In order to gain some understanding of the nature of these losses, a single-cell cavity has been tested in the TM_{010} and TE_{011} modes at 2 K. The feature of the TE_{011} mode is to have zero electric field on the cavity surface, so that electric field effects can be excluded as a source for the Q drop. This article will present some of the experimental results for different cavity treatments and will compare them with existing models. |
url |
http://doi.org/10.1103/PhysRevSTAB.9.042001 |
work_keys_str_mv |
AT gianluigiciovati measurementofthehighfieldqdropinthetm010andte011modesinaniobiumcavity AT peterkneisel measurementofthehighfieldqdropinthetm010andte011modesinaniobiumcavity |
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