“…The beam envelope that determines the outer radius of the equilibrium beam around the centroid is shown to obey the familiar envelope equation [6,8,15,16], being independent of the centroid motion. An example of the Vlasov equilibrium is discussed in detail to show the possibility of finding beam solutions for which the extensively studied envelope equation [4,5,[9][10][11]17] is stable, whereas the centroid motion is unstable, revealing the importance of the centroid motion to overall beam confinement properties.We consider a free, continuous charged-particle beam propagating with average axial velocity b cê z through a periodic solenoidal focusing magnetic field described bywhere r xê x yê y , r x 2 y 2 1=2 is the radial distance from the field symmetry axis, s z b ct is the axial coordinate, B z s S B z s is the magnetic field on the axis, the prime denotes derivative with respect to s, c is the speed of light in vacuo, and S is the periodicity length of the magnetic focusing field. Since we are dealing with solenoidal focusing, it is convenient to work in the Larmor frame of reference [8], which rotates with respect to the laboratory frame with angular velocity L s qB z s=2 b mc, where q, m, and b 1 ÿ 2 b ÿ1=2 are, respectively, the charge, mass, and relativistic factor of the beam particles.…”