Difference between revisions of "More information can be found here"
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The following is the LHRS matrix optimized by GMp | The following is the LHRS matrix optimized by GMp | ||
− | [ | + | [3] [http://web.mit.edu/reynier/www/Tritium_optics_matrices/LHRS_GMp_optics.html LHRS GMp optimization] |
The following is an optimization that Shujie did on the GMp LHRS matrix [3] | The following is an optimization that Shujie did on the GMp LHRS matrix [3] | ||
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The following is the RHRS matrix optimized by GMp | The following is the RHRS matrix optimized by GMp | ||
− | [ | + | [5] [http://web.mit.edu/reynier/www/Tritium_optics_matrices/RHRS_GMp_optics.html RHRS GMp optimization] |
= Current (optimized) matrices = | = Current (optimized) matrices = |
Revision as of 15:14, 26 July 2018
Contents
Old matrices
The following are the matrices that we used during the online analysis of the experiment:
[HERE] [1]
[HERE] [2]
Optimization steps
LHRS
The following is the LHRS matrix optimized by GMp
The following is an optimization that Shujie did on the GMp LHRS matrix [3] using the standard procedure for optimizing the angles and the sieve runs taken during MARATHON
[HERE] [4]
RHRS
The following is the RHRS matrix optimized by GMp
Current (optimized) matrices
LHRS
Replaced in matrix [4] the line:
D 1 0 0 -6.863500E-02 2.633700E-01 1.096600E-02 -7.253300E-02
with:
D 1 0 0 4.932426E-03 2.633700E-01 1.096600E-02 -7.253300E-02
This is the coefficient that relates delta with theta (xptar) fp linearly. We did this to get rid of a slope we saw in Emiss vs. xptar.
RHRS
Replaced in matrix [5] the line:
D 0 0 0 1.816209E-03 8.382911E-02 7.297953E-03 3.822568E-03 1.149510E-02
with:
D 0 0 0 0.000000E+00 8.382911E-02 7.297953E-03 3.822568E-03 1.149510E-02
and added the following two lines:
T 0 0 0 -2.940000E-03
P 0 0 0 -1.567257E-03