Two different parameters for the quantitative description of beam halo are introduced, both based on moments of the particle distribution. One parameter is a measure of spatial halo formation and has been defined previously by Wangler and Crandall [3], termed the profile parameter. The second parameter relies on kinematic invariants to quantify halo formation in phase space; we call it the halo parameter. The profile parameter can be computed from experimental beam profile data. The halo parameter provides a theoretically more complete description of halo in phase space, but is difficult to obtain experimentally
Beam profile (emittance) and beam halo are characteristic properties of high-intensity and high ener...
We recently constructed, analytically and numerically, a new class of self-consistent 6-D phase spac...
We report macroparticle simulations for comparison with measured results from a proton beam-halo ex...
Two different parameters for the quantitative description of beam halo are discussed. Both are based...
The characterization of the beam distribution at the exit of a high intensity RFQ is a crucial point...
We propose a model-independent quantity, L/G, to characterize non-Gaussian tails in beam profiles ob...
In this paper we review the present picture of km halo in proton linacs. Space-charge forces acting ...
Beam halo measurements imply measurements of beam profiles with a very high dynamic range; in transv...
Random phcnomcnoms like coulomb scattering or synchrotron radiation increases the transverse mittanc...
A realistic treatment of halo formation must take into account 3D beam bunches and 6D phase space di...
We present an overview of the status of ongoing work on physics models describing beam matching and ...
We compare macroparticle simulations with beam-profile measurements from a proton beam-halo experime...
We present an overview of the status of ongoing work on physics models describing beam matching and ...
We compare macroparticle simulations with beam-profile measurements from a proton beam-halo experime...
The effect of an initial envelope mismatch on the transport of bunched spherically symmetric beams i...
Beam profile (emittance) and beam halo are characteristic properties of high-intensity and high ener...
We recently constructed, analytically and numerically, a new class of self-consistent 6-D phase spac...
We report macroparticle simulations for comparison with measured results from a proton beam-halo ex...
Two different parameters for the quantitative description of beam halo are discussed. Both are based...
The characterization of the beam distribution at the exit of a high intensity RFQ is a crucial point...
We propose a model-independent quantity, L/G, to characterize non-Gaussian tails in beam profiles ob...
In this paper we review the present picture of km halo in proton linacs. Space-charge forces acting ...
Beam halo measurements imply measurements of beam profiles with a very high dynamic range; in transv...
Random phcnomcnoms like coulomb scattering or synchrotron radiation increases the transverse mittanc...
A realistic treatment of halo formation must take into account 3D beam bunches and 6D phase space di...
We present an overview of the status of ongoing work on physics models describing beam matching and ...
We compare macroparticle simulations with beam-profile measurements from a proton beam-halo experime...
We present an overview of the status of ongoing work on physics models describing beam matching and ...
We compare macroparticle simulations with beam-profile measurements from a proton beam-halo experime...
The effect of an initial envelope mismatch on the transport of bunched spherically symmetric beams i...
Beam profile (emittance) and beam halo are characteristic properties of high-intensity and high ener...
We recently constructed, analytically and numerically, a new class of self-consistent 6-D phase spac...
We report macroparticle simulations for comparison with measured results from a proton beam-halo ex...