Difference between revisions of "More information can be found here"
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([https://hallaweb.jlab.org/wiki/index.php/He3_/_H3_e%2Ce%27p_experiment_E12-14-011 BACK TO THE MAIN PAGE]) | ([https://hallaweb.jlab.org/wiki/index.php/He3_/_H3_e%2Ce%27p_experiment_E12-14-011 BACK TO THE MAIN PAGE]) | ||
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+ | = Old matrices = | ||
The following are the matrices that we used during the online analysis of the experiment: | The following are the matrices that we used during the online analysis of the experiment: |
Revision as of 15:07, 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
[HERE] [3]
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
[HERE] [5]
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