[BTeam] Lambertson multipoles
Jay Benesch
benesch at jlab.org
Sun Apr 24 16:03:22 EDT 2016
In late 2014 I modeled the Lambertson at Arne's request.
https://jlabdoc.jlab.org/docushare/dsweb/Get/Document-10105/15-005.pdf
There is a large skew quad and a significant normal sextupole resulting
from the Lambertson in all beam paths, but Hall B suffers most from skew
quad as HPS demonstrated. Mike Tiefenback recently asked me to design a
Panofsky quad with could be mounted to null the Lambertson skew quad.
See results in
https://jlabdoc.jlab.org/docushare/dsweb/Get/Document-117253/16-007.pdf
BPMs were installed between the vertical MBDs over a decade ago at the
suggestion of Johan Bengttson. I must have been asleep during the
discussion because the beams are not supposed to be at zero vertically
in the A and C lines until C01 girder, after the MBDs take out the
residual vertical angle from the transport recombiner. Steering to zero
at C00 screws up steering downstream.
In response to Mike's query I decided to spend ~700 CPU hours
calculating the fields in the Lambertson for all combinations of A and C
passes, 25 in all. The paths used to calculate multipoles were started
at A (0,2.2,-150) ; B (0,0,-150) ; C (0,-2.2,-150) even though the A and
C beam pipes in the Lambertson are horizontally offset from zero by by
about +- 0.35 cm. Ops doesn't offset the A and C beams from the center
of Lambertson viewer - it stacks them in a vertical line. I attempted
neither to get the entrance heights nor the angles for each pass right
at z=-150; I used one orbit parallel to the Z axis starting at the
indicated locations in calculating multipoles. Since I have the full
field models I could get fancier if someone can convince me the effort
would be worthwhile.
Since the A and C channels are offset from zero and the orbits I chose
are not, I calculated all 25 combinations rather than just the 15
on/above the diagonal. Decide for yourself from the attached whether
the offsets are significant.
I suggest the the B team consider installing girders consisting of
relocated BPMs, Panofsky skew quads, and sextupoles relocated from C08
girders about midway between the Lambertson and C01 girders. BPMs would
be zeroed via the Panofsky quads and the design vertical offset at that
location then put in GOF so Ops could steer to zero on C00 and C01
girders using the MBDxC00V correctors. Skew quad and normal sextupole
would be set according to my Lambertson model results. For conventional
solenoids, dipoles and the combined function PEPPo spectrometer my
models agree with measurement to better than 0.25%; for the multipoles
I'd estimate 5%. Nulling skew quadrupole and normal sextupole within 5%
will improve matching and beam quality.
If you deem the effort superfluous, it was only about a day of my time
and 100 kWh wasted.
Jay
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