KSBEND

A kick bending magnet which is NOT canonical, but is better than a 2nd order matrix implementation. Recommend using CSBEND instead.
Parallel capable? : yes

Parameter Name	Units	Type	Default	Description
L	$M$	double	0.0	arc length
ANGLE	$RAD$	double	0.0	bend angle
K1	$1/M^{2}$	double	0.0	geometric quadrupole strength
K2	$1/M^{3}$	double	0.0	geometric sextupole strength
K3	$1/M^{4}$	double	0.0	geometric octupole strength
K4	$1/M^{5}$	double	0.0	geometric decapole strength
E1	$RAD$	double	0.0	entrance edge angle
E2	$RAD$	double	0.0	exit edge angle
TILT	$RAD$	double	0.0	rotation about incoming longitudinal axis
H1	$1/M$	double	0.0	entrance pole-face curvature
H2	$1/M$	double	0.0	exit pole-face curvature
HGAP	$M$	double	0.0	half-gap between poles
FINT		double	0.5	edge-field integral
DX	$M$	double	0.0	misalignment
DY	$M$	double	0.0	misalignment
DZ	$M$	double	0.0	misalignment
FSE		double	0.0	fractional strength error
ETILT	$RAD$	double	0.0	error rotation about incoming longitudinal axis
N_KICKS		long	4	number of kicks
NONLINEAR		long	1	include nonlinear field components?
SYNCH_RAD		long	0	include classical synchrotron radiation?
EDGE1_EFFECTS		long	1	include entrance edge effects?
EDGE2_EFFECTS		long	1	include exit edge effects?
EDGE_ORDER		long	1	edge matrix order
PARAXIAL		long	0	use paraxial approximation?
TRANSPORT		long	0	use (incorrect) TRANSPORT equations for T436 of edge?
METHOD		STRING	modified-midpoint	integration method (modified-midpoint, leap-frog

A kick bending magnet which is NOT canonical, but is better than a 2nd order matrix implementation. Recommend using CSBEND instead.

Parameter Name	Units	Type	Default	Description
GROUP		string	NULL	Optionally used to assign an element to a group, with a user-defined name. Group names will appear in the parameter output file in the column ElementGroup