Standard

Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide. / Alekhina, T.Y.; Tyukhtin, A.V.

In: Physical Review Special Topics - Accelerators and Beams, Vol. 17, No. 7, 2014, p. 071302_1-8.

Research output: Contribution to journal › Article

Harvard

Alekhina, TY & Tyukhtin, AV 2014, 'Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide', Physical Review Special Topics - Accelerators and Beams, vol. 17, no. 7, pp. 071302_1-8. https://doi.org/10.1103/PhysRevSTAB.17.071302

APA

Alekhina, T. Y., & Tyukhtin, A. V. (2014). Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide. Physical Review Special Topics - Accelerators and Beams, 17(7), 071302_1-8. https://doi.org/10.1103/PhysRevSTAB.17.071302

Vancouver

Alekhina TY, Tyukhtin AV. Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide. Physical Review Special Topics - Accelerators and Beams. 2014;17(7):071302_1-8. https://doi.org/10.1103/PhysRevSTAB.17.071302

Author

Alekhina, T.Y. ; Tyukhtin, A.V. / Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide. In: Physical Review Special Topics - Accelerators and Beams. 2014 ; Vol. 17, No. 7. pp. 071302_1-8.

BibTeX

@article{cc015dfeedd04998bd78589c982d87a2,
title = "Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide",
abstract = "The electromagnetic field of a bunch moving through a vacuum gap located in a dielectric loaded waveguide is under investigation. This paper focuses on the case when Cherenkov radiation is generated in the dielectric parts of the waveguide. Analysis of the field components of the waveguide mode is performed both analytically and numerically, and the electromagnetic field structure for different time moments and different gap lengths is demonstrated. In particular, it is shown that for dielectrics with permittivity ε <2, the field of the ultrarelativistic bunch can be restored in the area after the vacuum gap for some optimal parameters of the problem. However, for dielectrics with ε > 2, restoration of the wakefield can only be realized for small lengths of the gap.",
author = "T.Y. Alekhina and A.V. Tyukhtin",
year = "2014",
doi = "10.1103/PhysRevSTAB.17.071302",
language = "English",
volume = "17",
pages = "071302_1--8",
journal = "Physical Review Special Topics - Accelerators and Beams",
issn = "1098-4402",
publisher = "American Physical Society",
number = "7",

}

RIS

TY - JOUR

T1 - Electromagnetic field of a bunch intersecting a vacuum gap in a dielectric loaded waveguide

AU - Alekhina, T.Y.

AU - Tyukhtin, A.V.

PY - 2014

Y1 - 2014

N2 - The electromagnetic field of a bunch moving through a vacuum gap located in a dielectric loaded waveguide is under investigation. This paper focuses on the case when Cherenkov radiation is generated in the dielectric parts of the waveguide. Analysis of the field components of the waveguide mode is performed both analytically and numerically, and the electromagnetic field structure for different time moments and different gap lengths is demonstrated. In particular, it is shown that for dielectrics with permittivity ε <2, the field of the ultrarelativistic bunch can be restored in the area after the vacuum gap for some optimal parameters of the problem. However, for dielectrics with ε > 2, restoration of the wakefield can only be realized for small lengths of the gap.

AB - The electromagnetic field of a bunch moving through a vacuum gap located in a dielectric loaded waveguide is under investigation. This paper focuses on the case when Cherenkov radiation is generated in the dielectric parts of the waveguide. Analysis of the field components of the waveguide mode is performed both analytically and numerically, and the electromagnetic field structure for different time moments and different gap lengths is demonstrated. In particular, it is shown that for dielectrics with permittivity ε <2, the field of the ultrarelativistic bunch can be restored in the area after the vacuum gap for some optimal parameters of the problem. However, for dielectrics with ε > 2, restoration of the wakefield can only be realized for small lengths of the gap.

U2 - 10.1103/PhysRevSTAB.17.071302

DO - 10.1103/PhysRevSTAB.17.071302

M3 - Article

VL - 17

SP - 071302_1-8

JO - Physical Review Special Topics - Accelerators and Beams

JF - Physical Review Special Topics - Accelerators and Beams

SN - 1098-4402

IS - 7

ER -

ID: 7009156