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Subsections
In HKS experiment, although the Splitter field smears the one to one
correspondence between target angles and sieve slit hole position and introduces additional momentum dependence.
particle trajectories scattered from a point target with given momenta
still have a fixed target angle when they pass a given hole.
The angle in this case is also a function of particle momentum, and
depend on splitter optics. Based on this observation, the Sieve slit
calibration procedure is:
- Fit function : target angles as a function of SS
positions and momentum based on Splitter optics.
- Separate events of the SS calibration run data hole by hole,
thus determine corresponding SS hole center
position for each event.
- Using function , calculate corrected target angles
(, ) for each event from SS center position and
momentum.
- Fit transfer matrix from focal plane to target: (, , ,
)
(, ).
A simulation of the SS calibration procedure with initial inaccurate
Splitter, Enge optics reaches final resolution for e' (Enge) target
angles (): : 1.8 mr, : 1.1 mr, for Kaon (HKS)
angles: : 0.4 mr, : 2.4 mr.
The codes are written in Perl script, which calls a series of Fortran
programs. Currently, they work on simulated data. All the
codes start from the
directory:jlabs1:/home/yuan/HKS/optics/
.enge/fsv2tarang
: Perl script to fit target angles as function
of sieve slit positions (, ) and momentum by 6-order
polynomials.
.enge/opticscalib
: Perl script to fit target angles as 6-order
polynomials of focal plane quantities.
- Nominal electron arm Raytrace data
card:
.enge/hksearm_tilt.dat
- nominal electron arm reconstruction matrix:
.enge/enge_recon_coeff.dat
Next: Momentum Calibration
Up: Hall C Expert Howto
Previous: General Procedure
Stephen A. Wood
2005-05-13