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Electromagnetic cavity Helmholtz equation
, 2012
"... Existence and uniqueness Finite element method a b s t r a c t Here considered is the mathematical analysis and numerical computation of the electromagnetic wave scattering by multiple cavities embedded in an infinite ground plane. Above the ground plane the space is filled with a homogeneous mediu ..."
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Existence and uniqueness Finite element method a b s t r a c t Here considered is the mathematical analysis and numerical computation of the electromagnetic wave scattering by multiple cavities embedded in an infinite ground plane. Above the ground plane the space is filled with a homogeneous
Potentials for a Rectangular Electromagnetic Cavity
"... Problem Deduce scalar and vector potentials relevant to electromagnetic modes in a rectangular cavity of dimensions d x ≥ d y ≥ d z , assuming the walls to be perfect conductors, and the interior of the cavity to be vacuum. Solution For the case of a cylindrical cavity, see E and B Fields of the C ..."
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Cited by 2 (2 self)
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Problem Deduce scalar and vector potentials relevant to electromagnetic modes in a rectangular cavity of dimensions d x ≥ d y ≥ d z , assuming the walls to be perfect conductors, and the interior of the cavity to be vacuum. Solution For the case of a cylindrical cavity, see E and B Fields
Shape determination for deformed electromagnetic cavities
 J. Comp. Phys
"... The measured physical parameters of a superconducting cavity differ from those of the designed ideal cavity. This is due to shape deviations caused by both loose machine tolerances during fabrication and by the tuning process for the accelerating mode. We present a shape determination algorithm to s ..."
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Cited by 3 (0 self)
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The measured physical parameters of a superconducting cavity differ from those of the designed ideal cavity. This is due to shape deviations caused by both loose machine tolerances during fabrication and by the tuning process for the accelerating mode. We present a shape determination algorithm
Potentials for a Cylindrical Electromagnetic Cavity
"... Deduce scalar and vector potentials relevant to the lowest electromagnetic mode in a right circular cylindrical cavity of radius R and axial extend 2D, assuming the walls to be perfect conductors, and the interior of the cavity to be vacuum. 2 Solution For the case of a rectangular cavity, see [1]. ..."
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Cited by 1 (1 self)
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Deduce scalar and vector potentials relevant to the lowest electromagnetic mode in a right circular cylindrical cavity of radius R and axial extend 2D, assuming the walls to be perfect conductors, and the interior of the cavity to be vacuum. 2 Solution For the case of a rectangular cavity, see [1
Experimental Study of Pulsed Heating of Electromagnetic Cavities
 in Proceedings of the 1997 Particle Accelerator Conference
, 1998
"... An experiment to study the effects of pulsed heating in electromagnetic cavities will be performed. Pulsed heating is believed to be the limiting mechanism of high acceleration gradients at short wavelengths. A cylindrical cavity operated in the TE011mode at a frequency of 11.424 GHz will be used. A ..."
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Cited by 4 (2 self)
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An experiment to study the effects of pulsed heating in electromagnetic cavities will be performed. Pulsed heating is believed to be the limiting mechanism of high acceleration gradients at short wavelengths. A cylindrical cavity operated in the TE011mode at a frequency of 11.424 GHz will be used
New Journal of Physics Creating electromagnetic cavities using transformation optics
, 2012
"... Creating electromagnetic cavities using transformation optics This article has been downloaded from IOPscience. Please scroll down to see the full text article. ..."
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Creating electromagnetic cavities using transformation optics This article has been downloaded from IOPscience. Please scroll down to see the full text article.
Twoatom dark states in electromagnetic cavities
"... The centerofmass motion of two twolevel atoms coupled to a single damped mode of an electromagnetic resonator is investigated. For the case of one atom being initially excited and the cavity mode in the vacuum state, it is shown that the atomic time evolution is dominated by the appearance of da ..."
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The centerofmass motion of two twolevel atoms coupled to a single damped mode of an electromagnetic resonator is investigated. For the case of one atom being initially excited and the cavity mode in the vacuum state, it is shown that the atomic time evolution is dominated by the appearance
The Viterbi algorithm
 Proceedings of the IEEE
, 1973
"... vol. 6, no. 8, pp. 211220, 1951. [7] J. L. Anderson and J. W..Ryon, “Electromagnetic radiation in accelerated systems, ” Phys. Rev., vol. 181, pp. 17651775, 1969. [8] C. V. Heer, “Resonant frequencies of an electromagnetic cavity in an accelerated system of reference, ” Phys. Reu., vol. 134, pp. A ..."
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Cited by 994 (3 self)
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vol. 6, no. 8, pp. 211220, 1951. [7] J. L. Anderson and J. W..Ryon, “Electromagnetic radiation in accelerated systems, ” Phys. Rev., vol. 181, pp. 17651775, 1969. [8] C. V. Heer, “Resonant frequencies of an electromagnetic cavity in an accelerated system of reference, ” Phys. Reu., vol. 134, pp
Excitation of a Rectangular Electromagnetic Cavity by a Passing, Relativistic Electron
"... Deduce the strength of the lowest mode of a rectangular electromagnetic cavity when excited by a relativistic electron of charge −e and speed v ≈ c, wherec is the speed of light in vacuum. The rectangular cavity has dimensions dx ≥ dy ≥ dz, and the electron moves parallel to the zaxis. The cavity w ..."
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Deduce the strength of the lowest mode of a rectangular electromagnetic cavity when excited by a relativistic electron of charge −e and speed v ≈ c, wherec is the speed of light in vacuum. The rectangular cavity has dimensions dx ≥ dy ≥ dz, and the electron moves parallel to the zaxis. The cavity
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