PLOT HIST, [NONEWPAGE,]
[RIGHTLEFT,]
[KIND=k
(
,
),]
[GENERATION rel n,] [INCP,]
H=
,
[HSCALE=(
,
,
),]
[HLOG,] [VLOG,]
[TITLE='head_title',]
[HTITLE='bottom_title',]
[VTITLE='left_title',]
[FILE=
,]
;
PLOT SCATTER, [NONEWPAGE,]
[RIGHTLEFT,]
[KIND=k
(
,
),]
[GENERATION rel n,] [INCP,]
H=
, V=
,
[HSCALE=(
,
),]
[VSCALE=(
,
),]
[HLOG,] [VLOG,] [MAXNP=
,]
[TITLE='top_title',]
[HTITLE='bottom_title',]
[VTITLE='left_title',]
[FILE=
,]
;
PLOT TESTPARTICLE, [RIGHTLEFT,]
[KIND=k
(
,
),]
H=
, V=
,
[HSCALE=(
,
),]
[VSCALE=(
,
),]
[TITLE='top_title',]
[HTITLE='bottom_title',]
[VTITLE='left_title',]
[FILE=
,]
;
Other operands are the same as for the scatter plot. Note that the
information of the test particle history is stored (in contrast to
normal particles). Thus, you can say, for example, H=T to see
the trajectory as a function of time.
The plot may show apparently unphysical features when you apply DRIFT command. DRIFT command may be used to pull particles to a certain position or time. This does not corresponds to a physical motion. Even in such cases, test particle coordinates are stored at the end of DRIFT command. Moreover, in contrast to the PUSH command, step-by-step information of test particles during DRIFT command is not stored because DRIFT command calculates particle trajectories by a single step using exact analytic formulas.
if defined by LUMINOSITY command and calculated by PUSH command.
PLOT LUMINOSITY,
[FILE=,] [VLOG,]
;
The charge distribution and the beam field data for beam-beam interaction are computed at each time step for each longitudinal slice but they are not kept in the memory. They can be plotted only at the time moment and for the slice which is being proccessed. Thus, this command is to be inserted during PUSH loop. The slice is specified by the S operand.
PLOT BBFIELD,
S=S=(
,
,
),
[FILE=
,]
;