Age | Commit message (Collapse) | Author |
|
|
|
This commit updates the estimate_errors() function so that it works
without a list of constraints and uses arrays of low and high bounds
passed in instead of hardcoded constraints.
I can now call this function from the chi2 analysis to get the stepsizes
before running the MCMC.
|
|
- delete instrumental tags in both scripts since we already tag them in
get_events()
- apply the same cuts to the MC as to the data
- add a comment about the fitted fraction
- quit if we don't have at least 1 type of each instrumental
|
|
|
|
memory
|
|
instrumentals
This commit updates the contamination analysis scripts to take into account the
fact that we only fit a fraction of some of the instrumental events.
Based on the recent rate at which my jobs have been running on the grid,
fitting all the events would take *way* too long. Therefore, I'm now planning
to only fit 10% of muon, flasher, and neck events. With this commit the
contamination analysis will now correctly take into account the fact that we
aren't fitting all the instrumental events.
|
|
This commit updates the step size used for the MCMC in the contamination
analysis to 0.5 times the error returned by scanning near the minimum. I ran
some tests and this seemed to be pretty efficient compared to either the full
error or 0.1 times the error. I also reduced the number of workers to 10.
|
|
- fix Constraint.renormalize_no_fix() which could enter an infinite loop if the
fixed parameter was greater than 1 - EPSILON
- don't divide by psi twice in get_events()
- only use prompt events and cut on nhit_cal < 100
|
|
|
|
|
|
This commit contains the following updates:
- remove hack to get rid of low energy events in plot-energy since while
writing the unidoc I realized it's not necessary now that we add +100 to
multi-particle fits
- update Ockham factor to use an energy resolution of 5%
- update submit-grid-jobs to submit jobs according to the following criteria:
- always submit prompt events with no data cleaning cuts
- submit 10% of prompt flasher events
- submit all other prompt events
- submit followers only if they have no data cleaning cuts
- update submit-grid-jobs to place the nhit cut of 100 on the calibrated nhit
|
|
This commit adds an sddm python package to the utils/ folder. This allows me to
consolidate code used across all the various scripts. This package is now
installed by default to /home/tlatorre/local/lib/python2.7/site-packages so you
should add the following to your .bashrc file:
export PYTHONPATH=$HOME/local/lib/python2.7/site-packages/:$PYTHONPATH
before using the scripts installed to ~/local/bin.
|
|
This commit updates the dc script to calculate the instrumental contamination
to now treat all 4 high level variables as correlated for muons. Previously I
had assumed that the reconstructed radius was independent from udotr, z, and
psi, but based on the corner plots it seems like the radius is strongly
correlated with udotr.
I also updated the plotting code when using the save command line argument to
be similar to plot-fit-results.
|
|
This commit adds a script to calculate the background contamination using a
method inspired by the bifurcated analysis method used in SNO. The method works
by looking at the distribution of several high level variables (radius, udotr,
psi, and reconstructed z position) for events tagged by the different data
cleaning cuts and assuming that any background events which sneak past the data
cleaning cuts will have a similar distribution (for certain backgrounds this is
assumed and for others I will actually test this assumption. For more details
see the unidoc). Then, by looking at the distribution of these high level
variables for all the untagged events we can use a maximum likelihood fit to
determine the residual contamination.
There are also a few other updates to the plot-energy script:
- add a --dc command line argument to plot corner plots for the high level
variables used in the contamination analysis
- add a fudge factor to the Ockham factor of 100 per extra particle
- fix a bug by correctly setting the final kinetic energy to the sum of the
individual kinetic energies instead of just the first particle
- fix calculation of prompt events by applying at the run level
|