Abstract
This paper provides a systematic derivation of a guiding-center kinetic model that describes intense beam propagation through a periodic focusing lattice with axial periodicity length $S$, valid for sufficiently small phase advance (say, $\ensuremath{\sigma}<60\ifmmode^\circ\else\textdegree\fi{}$). The analysis assumes a thin $(a,b\ensuremath{\ll}S)$ axially continuous beam, or very long charge bunch, propagating in the $z$ direction through a periodic focusing lattice with transverse focusing coefficients ${\ensuremath{\kappa}}_{x}(s+S)\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}{\ensuremath{\kappa}}_{x}(s)$ and ${\ensuremath{\kappa}}_{y}(s+S)\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}{\ensuremath{\kappa}}_{y}(s)$, where $S\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}\mathrm{const}$ is the lattice period. By averaging over the (fast) oscillations occurring on the length scale of a lattice period $S$, the analysis leads to smooth-focusing Vlasov-Maxwell equations that describe the slow evolution of the guiding-center distribution function ${\overline{f}}_{b}(\overline{x},\overline{y},{\overline{x}}^{\ensuremath{'}},{\overline{y}}^{\ensuremath{'}},s)$ and (normalized) self-field potential $\overline{\ensuremath{\psi}}(\overline{x},\overline{y},s)$ in the four-dimensional transverse phase space $(\overline{x},\overline{y},{\overline{x}}^{\ensuremath{'}},{\overline{y}}^{\ensuremath{'}})$. In the resulting kinetic equation for ${\overline{f}}_{b}(\overline{x},\overline{y},{\overline{x}}^{\ensuremath{'}},{\overline{y}}^{\ensuremath{'}},s)$, the average effects of the applied focusing field are incorporated in constant focusing coefficients ${\ensuremath{\kappa}}_{x\mathrm{sf}}>0$ and ${\ensuremath{\kappa}}_{y\mathrm{sf}}>0$, and the model is readily accessible to direct analytical investigation. Similar smooth-focusing Vlasov-Maxwell descriptions are widely used in the accelerator physics literature, often without a systematic justification, and the present analysis is intended to place these models on a rigorous, yet physically intuitive, foundation.
Highlights
Periodic focusing accelerators and transport systems [1–9] have a wide range of applications ranging from basic scientific research in high energy and nuclear physics to applications such as coherent radiation sources, heavy ion fusion, tritium production, nuclear waste transmutation, and spallation neutron sources for materials and biological research [10,11]
The purpose of this article is to provide a systematic derivation of a guiding-center kinetic model that describes intense beam propagation through a periodic focusing lattice with period S, valid for sufficiently small phase advance
By averaging over the oscillations occurring on the length scale of a lattice period S, the analysis leads to smoothfocusing Vlasov-Maxwell equations describing the slow evolution of the guiding-center distribution function fbx, y, x 0, y 0, sand self-field potential cx, y, sin the four-dimensional transverse phase spacex, y, x 0, y 0͒
Summary
Periodic focusing accelerators and transport systems [1–9] have a wide range of applications ranging from basic scientific research in high energy and nuclear physics to applications such as coherent radiation sources, heavy ion fusion, tritium production, nuclear waste transmutation, and spallation neutron sources for materials and biological research [10,11]. The purpose of this article is to provide a systematic derivation of a guiding-center kinetic model that describes intense beam propagation through a periodic focusing lattice with period S, valid for sufficiently small phase advance (say, s , 60±). By averaging over the (fast) oscillations occurring on the length scale of a lattice period S, the analysis leads to smoothfocusing Vlasov-Maxwell equations describing the slow evolution of the guiding-center distribution function fbx , y , x 0, y 0, sand (normalized) self-field potential c ͑x , y , sin the four-dimensional transverse phase spacex , y , x 0, y 0͒. While smooth-focusing VlasovMaxwell equations similar to Eqs. (57) and (58) are widely used in the accelerator physics literature [14], often without a systematic justification, a primary purpose of this paper is to place Eqs. (57) and (58) on a rigorous, yet physically intuitive, foundation
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have