1971IEEE Transactions on Nuclear ScienceRequires access

A Fast Beam Quality Measuring Device

W. A. van Kampen, J. Liedorp

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Abstract

A device has been designed and built to obtain the four dimensional emittance of a particle beam. Two rotating discs with hole patterns scan the beam using the Nipkov principle. The emittance is determined from 10.000 beam samples, each of which is taken in 1 ms. Dependent on the chosen hole pattern a complete cycle of 10.000 samples takes 20-40 s. A small computer is used to control the experiment and to store the measurement data. Beam samples of 1 nA and up can be measured with 1% accuracy. The emittance of a particle beam can be described as a function in the four dimensional phase space: E(x,x',y,y'), with E = dI/dV, where x and y are mutually perpendiculat and transverse to the beam direction z, I is the beam current, dV a volume element in phase space, and x' = dx/dz, y' = dy/dz. A much used representation of the emittance is given by E(x,x') = ∫ Edydy', E(y,y') = ∫ Edxdx'. phase space phase space

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A device has been designed and built to obtain the four dimensional emittance of a particle beam. Two rotating discs with hole patterns scan the beam using the Nipkov principle. The emittance is determined from 10.000 beam samples, each of which is taken in 1 ms. Dependent on the chosen hole pattern a complete cycle of 10.000 samples takes 20-40 s. A small computer is used to control the experiment and to store the measurement data. Beam samples of 1 nA and up can be measured with 1% accuracy. The emittance of a particle beam can be described as a function in the four dimensional phase space: E(x,x',y,y'), with E = dI/dV, where x and y are mutually perpendiculat and transverse to the beam direction z, I is the beam current, dV a volume element in phase space, and x' = dx/dz, y' = dy/dz. A much used representation of the emittance is given by E(x,x') = ∫ Edydy', E(y,y') = ∫ Edxdx'. phase space phase space

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Available abstract

A device has been designed and built to obtain the four dimensional emittance of a particle beam. Two rotating discs with hole patterns scan the beam using the Nipkov principle. The emittance is determined from 10.000 beam samples, each of which is taken in 1 ms. Dependent on the chosen hole pattern a complete cycle of 10.000 samples takes 20-40 s. A small computer is used to control the experiment and to store the measurement data. Beam samples of 1 nA and up can be measured with 1% accuracy. The emittance of a particle beam can be described as a function in the four dimensional phase space: E(x,x',y,y'), with E = dI/dV, where x and y are mutually perpendiculat and transverse to the beam direction z, I is the beam current, dV a volume element in phase space, and x' = dx/dz, y' = dy/dz. A much used representation of the emittance is given by E(x,x') = ∫ Edydy', E(y,y') = ∫ Edxdx'. phase space phase space

Key concepts: Thermal emittance, Beam emittance, Beam (structure), Physics, Laser beam quality, Optics, Phase space, Particle accelerator

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