A magnet with multipoles. Note that the reference plane is defined so that the skew quadrupole component becomes zero. It can have a nonzero ANGLE to express a combined funtion bending magnet with multipoles. Note that the definition of the multipoles with nonzero ANGLE is very special The current version does not allow nonzero ANGLE inside a solenoid or with acceleration. Also the fringe field and emittance calculation are not installed properly for nonzero ANGLE.
DISFRIN=0 DISFRIN<>0
Nonlinear Linear Nonlinear Linear
FRINGE=0 entr & exit none none none
FRINGE=1 entr entr none entr
FRINGE=2 exit exit none exit
FRINGE=3 entr & exit entr & exit none entr & exitwhere ts is the equilibrium time determined by the valance between the acceleration and the radiation loss around the ring. DPHI is not taken into account to determine the design mementum p0(s).
with
where s0 is the location of the edge where the effective length is defined, and K1_0 is the nominal value of K1, given by the keyword K1. The effects only in the first ordef of K1 is taken into account.
where ts is the equilibrium time determined by the valance between the acceleration and the radiation loss around the ring. (CAVI only) The non-relativistic corrections
are automatically added to V20 and V02, respectively. The Lorentz factor is evaluated as inverse of average of
at the entrance
and the exit. DISFRIN=0 DISFRIN<>0
Nonlinear Linear Nonlinear Linear
FRINGE=0 entr & exit none none none
FRINGE=1 entr entr none entr
FRINGE=2 exit exit none exit
FRINGE=3 entr & exit entr & exit none entr & exitwhere L is the length of the component. Positive sign means horizontal focusing.
\begin{pmatrix}
x \\ y \\ ds\end{pmatrix}_{ 1}
=\begin{pmatrix}
c3 & -s3 & 0 \\ s3 & c3 & 0 \\ 0 & 0 & 1\end{pmatrix} \begin{pmatrix}
1 & 0 & 0 \\ 0 & c2 & -s2 \\ 0 & s2 & c2\end{pmatrix} \begin{pmatrix}
c1 & 0 & -s1 \\ 0 & 1 & 0 \\ s1 & 0 & c1\end{pmatrix} \begin{pmatrix}
x-DX \\ y-DY \\ -DZ\end{pmatrix} }} , where c1 and s1 are Cos[CHI1] and Sin[CHI1], etc. The inverse is applied at the exit. Those misalignments are also valid within a solenoid. Other straight elements such as QUAD or THIN do not and will not have these full misalignment specifications, because they can be substituted by MULT. The geometry of the design orbit are determined by the saved values of CHI1, CHI2, and DZ, while the current values are used for DX, DY, and ROTATE.
with
where
. Actually the summation is truncated at n + k <= 21
in the current version. While this definition converges to the regular
one for multipoles when ANGLE -> 0, K0 and K1 of MUILT are
different from those of BEND.where ts is the equilibrium time determined by the valance between the acceleration and the radiation loss around the ring.
where L is the length of the component. Positive sign means a horizontally focusing magnet rotated around z-axis by -90/(n+1) degree, i.e., ROTATE = (90/(n+1)) DEG.
where ts is the equilibrium time determined by the valance between the acceleration and the radiation loss around the ring.