Cavity beam position monitor system for the Accelerator Test Facility 2. / Kim, Y.I. ; Ainsworth, R.; Aryshev, A.; Boogert, S.T.; Boorman, G.; Frisch, J.; Heo, A; Honda, Y.; Hwang, W. H.; Huang, J Y ; Kim, E. -S.; Kim, S.H; Lyapin, A.; Naito, T.; May, J.; McCormick, D.; Mellor, R.E.; Molloy, S.; Nelson, J.; Park, S. J.; Park, Y.J; Ross, M.; Shin, S; Swinson, C.; Smith, T.; Terunuma, N.; Tauchi, T.; Urakawa, J.; White, G.R.

In: Physical Review Special Topics: Accelerators and Beams, Vol. 15, No. 4, 042801, 10.04.2012.

Research output: Contribution to journalArticle

Published

Standard

Cavity beam position monitor system for the Accelerator Test Facility 2. / Kim, Y.I. ; Ainsworth, R.; Aryshev, A.; Boogert, S.T.; Boorman, G.; Frisch, J.; Heo, A; Honda, Y.; Hwang, W. H.; Huang, J Y ; Kim, E. -S.; Kim, S.H; Lyapin, A.; Naito, T.; May, J.; McCormick, D.; Mellor, R.E.; Molloy, S.; Nelson, J.; Park, S. J.; Park, Y.J; Ross, M.; Shin, S; Swinson, C.; Smith, T.; Terunuma, N.; Tauchi, T.; Urakawa, J.; White, G.R.

In: Physical Review Special Topics: Accelerators and Beams, Vol. 15, No. 4, 042801, 10.04.2012.

Research output: Contribution to journalArticle

Harvard

Kim, YI, Ainsworth, R, Aryshev, A, Boogert, ST, Boorman, G, Frisch, J, Heo, A, Honda, Y, Hwang, WH, Huang, JY, Kim, E-S, Kim, SH, Lyapin, A, Naito, T, May, J, McCormick, D, Mellor, RE, Molloy, S, Nelson, J, Park, SJ, Park, YJ, Ross, M, Shin, S, Swinson, C, Smith, T, Terunuma, N, Tauchi, T, Urakawa, J & White, GR 2012, 'Cavity beam position monitor system for the Accelerator Test Facility 2', Physical Review Special Topics: Accelerators and Beams, vol. 15, no. 4, 042801. https://doi.org/10.1103/PhysRevSTAB.15.042801

APA

Kim, Y. I., Ainsworth, R., Aryshev, A., Boogert, S. T., Boorman, G., Frisch, J., Heo, A., Honda, Y., Hwang, W. H., Huang, J. Y., Kim, E. -S., Kim, S. H., Lyapin, A., Naito, T., May, J., McCormick, D., Mellor, R. E., Molloy, S., Nelson, J., ... White, G. R. (2012). Cavity beam position monitor system for the Accelerator Test Facility 2. Physical Review Special Topics: Accelerators and Beams, 15(4), [042801]. https://doi.org/10.1103/PhysRevSTAB.15.042801

Vancouver

Kim YI, Ainsworth R, Aryshev A, Boogert ST, Boorman G, Frisch J et al. Cavity beam position monitor system for the Accelerator Test Facility 2. Physical Review Special Topics: Accelerators and Beams. 2012 Apr 10;15(4). 042801. https://doi.org/10.1103/PhysRevSTAB.15.042801

Author

Kim, Y.I. ; Ainsworth, R. ; Aryshev, A. ; Boogert, S.T. ; Boorman, G. ; Frisch, J. ; Heo, A ; Honda, Y. ; Hwang, W. H. ; Huang, J Y ; Kim, E. -S. ; Kim, S.H ; Lyapin, A. ; Naito, T. ; May, J. ; McCormick, D. ; Mellor, R.E. ; Molloy, S. ; Nelson, J. ; Park, S. J. ; Park, Y.J ; Ross, M. ; Shin, S ; Swinson, C. ; Smith, T. ; Terunuma, N. ; Tauchi, T. ; Urakawa, J. ; White, G.R. / Cavity beam position monitor system for the Accelerator Test Facility 2. In: Physical Review Special Topics: Accelerators and Beams. 2012 ; Vol. 15, No. 4.

BibTeX

@article{7b87c4b90e8d4d8daabee6cadcbdf714,
title = "Cavity beam position monitor system for the Accelerator Test Facility 2",
abstract = "The Accelerator Test Facility 2 (ATF2) is a scaled demonstrator system for final focus beam lines of linear high energy colliders. This paper describes the high resolution cavity beam position monitor (BPM) system, which is a part of the ATF2 diagnostics. Two types of cavity BPMs are used, C-band operating at 6.423 GHz, and S-band at 2.888 GHz with an increased beam aperture. The cavities, electronics, and digital processing are described. The resolution of the C-band system with attenuators was determined to be approximately 250 nm and 1  μm for the S-band system. Without attenuation the best recorded C-band cavity resolution was 27 nm.",
author = "Y.I. Kim and R. Ainsworth and A. Aryshev and S.T. Boogert and G. Boorman and J. Frisch and A Heo and Y. Honda and Hwang, {W. H.} and Huang, {J Y} and Kim, {E. -S.} and S.H Kim and A. Lyapin and T. Naito and J. May and D. McCormick and R.E. Mellor and S. Molloy and J. Nelson and Park, {S. J.} and Y.J Park and M. Ross and S Shin and C. Swinson and T. Smith and N. Terunuma and T. Tauchi and J. Urakawa and G.R. White",
year = "2012",
month = apr,
day = "10",
doi = "10.1103/PhysRevSTAB.15.042801",
language = "English",
volume = "15",
journal = "Physical Review Special Topics: Accelerators and Beams",
issn = "1098-4402",
publisher = "American Physical Society",
number = "4",

}

RIS

TY - JOUR

T1 - Cavity beam position monitor system for the Accelerator Test Facility 2

AU - Kim, Y.I.

AU - Ainsworth, R.

AU - Aryshev, A.

AU - Boogert, S.T.

AU - Boorman, G.

AU - Frisch, J.

AU - Heo, A

AU - Honda, Y.

AU - Hwang, W. H.

AU - Huang, J Y

AU - Kim, E. -S.

AU - Kim, S.H

AU - Lyapin, A.

AU - Naito, T.

AU - May, J.

AU - McCormick, D.

AU - Mellor, R.E.

AU - Molloy, S.

AU - Nelson, J.

AU - Park, S. J.

AU - Park, Y.J

AU - Ross, M.

AU - Shin, S

AU - Swinson, C.

AU - Smith, T.

AU - Terunuma, N.

AU - Tauchi, T.

AU - Urakawa, J.

AU - White, G.R.

PY - 2012/4/10

Y1 - 2012/4/10

N2 - The Accelerator Test Facility 2 (ATF2) is a scaled demonstrator system for final focus beam lines of linear high energy colliders. This paper describes the high resolution cavity beam position monitor (BPM) system, which is a part of the ATF2 diagnostics. Two types of cavity BPMs are used, C-band operating at 6.423 GHz, and S-band at 2.888 GHz with an increased beam aperture. The cavities, electronics, and digital processing are described. The resolution of the C-band system with attenuators was determined to be approximately 250 nm and 1  μm for the S-band system. Without attenuation the best recorded C-band cavity resolution was 27 nm.

AB - The Accelerator Test Facility 2 (ATF2) is a scaled demonstrator system for final focus beam lines of linear high energy colliders. This paper describes the high resolution cavity beam position monitor (BPM) system, which is a part of the ATF2 diagnostics. Two types of cavity BPMs are used, C-band operating at 6.423 GHz, and S-band at 2.888 GHz with an increased beam aperture. The cavities, electronics, and digital processing are described. The resolution of the C-band system with attenuators was determined to be approximately 250 nm and 1  μm for the S-band system. Without attenuation the best recorded C-band cavity resolution was 27 nm.

U2 - 10.1103/PhysRevSTAB.15.042801

DO - 10.1103/PhysRevSTAB.15.042801

M3 - Article

VL - 15

JO - Physical Review Special Topics: Accelerators and Beams

JF - Physical Review Special Topics: Accelerators and Beams

SN - 1098-4402

IS - 4

M1 - 042801

ER -