1961
DOI: 10.1080/00207216108937309
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Brillouin Flow in Relativistic Beams†

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Cited by 14 publications
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“…Equation (9) then allows one to express A z in terms of ', with eq ÀcH =H as the common longitudinal velocity of all beam particles. Therefore, regardless of the density profile across the beam, we find that the longitudinal speed at equilibrium follows a uniform distribution as a function of the radial coordinate [1,7]. Since it is possible to express A z in terms of ', convenient handling of the constant Hamiltonian H defined by expression (1) allows one to write the scalar potential ' entirely in terms of the azimuthal component of the vector potential, 'ðrÞ ¼ '½A ðrÞ.…”
Section: Review Of Equilibrium Statesmentioning
confidence: 93%
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“…Equation (9) then allows one to express A z in terms of ', with eq ÀcH =H as the common longitudinal velocity of all beam particles. Therefore, regardless of the density profile across the beam, we find that the longitudinal speed at equilibrium follows a uniform distribution as a function of the radial coordinate [1,7]. Since it is possible to express A z in terms of ', convenient handling of the constant Hamiltonian H defined by expression (1) allows one to write the scalar potential ' entirely in terms of the azimuthal component of the vector potential, 'ðrÞ ¼ '½A ðrÞ.…”
Section: Review Of Equilibrium Statesmentioning
confidence: 93%
“…To address the issue, we simulate the full set of equations (2)- (7). Small perveances are assumed, which implies that the paraxial approximation jdr=dzj ( 1 is valid, as long as emittance is also small enough so as not to push initially paraxial particles into nonparaxial orbits.…”
Section: Numerical Methods For Dynamicsmentioning
confidence: 99%
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