INTERPRETATION OF THE CONNECTING LINES IN THE PROJECTIONAL XX' EMITTANCE IN VIEW OF LIOUVILLES THEOREM

Authors
Citation
M. Sarstedt, INTERPRETATION OF THE CONNECTING LINES IN THE PROJECTIONAL XX' EMITTANCE IN VIEW OF LIOUVILLES THEOREM, Review of scientific instruments, 68(8), 1997, pp. 3036-3041
Citations number
9
Categorie Soggetti
Physics, Applied","Instument & Instrumentation
ISSN journal
00346748
Volume
68
Issue
8
Year of publication
1997
Pages
3036 - 3041
Database
ISI
SICI code
0034-6748(1997)68:8<3036:IOTCLI>2.0.ZU;2-B
Abstract
For the analytical and numerical description of the emittance of a par ticle beam in cylindrical symmetric transport and accelerator systems often the rr' plane is used, yielding a sectional emittance epsilon (r , r'). In contrast, emittance measurements are mostly taken as the pro jectional emittance epsilon (x, x'). As could be shown earlier, the de scription of a cylindrical symmetric beam in the projectional xx' plan e of phase space results in the presence of lines for each ring of par ticles, connecting the two corresponding points, with which the same b eam is described in the rr' plane. There is a very special intensity d istribution along these lines, both for straight as well as for skew t rajectories. It is shown here that the theoretically obtained density distribution along such a line is a weight function for the intensity measured with a slit of width Delta x. For one particle it can also be interpreted as a probability function for the particle being at a cer tain position x(0). In view of Liouville's theorem, the case of the tw o-dimensional emittance in cylindrical symmetric systems is discussed, where this law of conservation is, due to the coupling of the x and y planes, not generally applicable. It is shown here that for an emitta nce measurement performed in the xx' plane, cart has to be taken when choosing the slit width, since a small Delta x yields a good spatial r esolution, but increases the risk of missing information in the center of each connecting line. (C) 1997 American Institute of Physics.