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Feb 2/23 PionLT/KaonLT Analysis Meeting Notes
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---------------------------------------------
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(Notes by GH and SJDK)
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Today: KaonLT will be discussed first
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Please remember to post your slides at:
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https://redmine.jlab.org/projects/kltexp/wiki/Kaon_LT_Meetings
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Present
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-------
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Regina - Stephen Kay, Garth Huber, Ali Usman, Alicia Postuma, Nathan Heinrich,
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Vijay Kumar
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JLab - Dave Gaskell
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Ohio - Jacob Murphy
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CSULA - Yeranuhi Ghandilyan, Konrad Aniol
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CUA - Richard Trotta, Tanja Horn
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FIU - Pete Markowitz
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Vijay Updates
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-------------
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Update on Q2=0.38 low epsilon Analysis
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- CT peak, one peak either side of prompt peak looks very different (more
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counts), one is 2 left of Prompt, other is 3 right of Prompt
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for LEFT-2 SHMS setting only
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- Possibly a different particle leaking in, but then why does this give
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peaks on both sides?
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- Should create 2D distributions to check this
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- Plot CT vs MM
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- CT vs Beta too
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- TH: some weird random peaks were seen in Fpi-2 as well, but only on one
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side, it is weird here to have weird peaks on both sides of prompt peak
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- DG: yes, we can place cuts to avoid these weird peaks in the random
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subtraction, but we should spend some effort to understand why they're
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weird first
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- -ve events in MM distribution after Dummy and Random subtraction, to right of
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neutron peak
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- Green - central
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- Red - left1
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- Black - left2
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- After dummy + random subtraction - over subtraction?
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- Wrong charge assumed in dummy subtraction or similar? *Check*
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- MM peak is also very off, wrong MM used?
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- neutron peak is at 0.89, this is off a lot!
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- Vijay thinks it is MMpi, could easily be MMK if using Richard's analysis
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though *Check*
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- Diamond cut on low epsilon data
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- Cut shown for central setting
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- DG: How was this done?
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- Script maybe overcomplicating it?
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- It should be a relatively straightforward set of cuts
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- TH: Often it is nearly impossible to be sure exactly what you're doing
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if a complicated script is used
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- Each plot you make, you should be able to *understand* exactly what is
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done to the data
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- Some ragged blue region, it looks like SHMS+HMS acceptance cuts not
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applied
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- important to set the diamond cut after applying other physics analysis
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cuts, apply to ALL three epsilon data, including low epsilon, for
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consistency
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- RefTime cuts for this data?
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- Originally said not set but then said it was, not 100% clear
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- Think it's set ok? *Verify*
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- t-binning
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- Need same t bins for all three epsilon settings
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- Lowest t bin will have nothing from left2
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- Similarly highest bin will be only left2!
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- Look at all statistics for three epsilons to determine t binning
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- Apply diamond cut to mid/high epsilon, and other physics cuts too, such
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as MM, etc. Want the t-coverage and statistics to correspond
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reasonably well to what will be seen in the final physics analysis
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- Data/SIMC comparison
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- No scaling applied to SIMC, and normalization comparison looks
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reasurringly good, as pion model should work very well at these
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low Q2
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- Pion model should be much better than kaon model to begin with
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- SIMC distribution broader than data in xptar
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- implies on some aperture in the simulation is "off"
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- Which though? Very hard to determine
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- This is a mystery
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- Dave G has already updated target geometry in SIMC so it isn't that
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- DG has no other suggestions, but notes that the same is seen in SIDIS
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- SHMS yptar distributions SIMC, Data have same width, but a slight shift
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indicating a small offset issue?
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Richard Updates
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---------------
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- Diamond cuts
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- Q2=5.5 looks good
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- Acceptance cut is applied, less ragged edges than what Vijay showed
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- script crashes for Q2=2.11, investigating
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- t binning
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- Apply all cuts
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- PID
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- CT
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- Only one epsilon shown, will have to show both epsilons after diamond cuts
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to determine optimal binning
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- t-distribution goes through zero (not allowed), lots of events at t>0
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- Centre/left look OK
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- Right PID looks bad
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- Still clearly getting pi/p leakthrough
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- Large delta background under lambdas that needs to be removed
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- Try to get a clean pion sample, normalise this to residual neutron peak
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with kaon PID
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- Subtract it off
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- Basically infer the shape of the pion background from selecting out
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clean pions
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- Likely have to similarly get a clean proton sample, and normalize to
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residual omega peak, to remove proton leakthrough
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- Something seems to have gone very wrong for the right setting
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*Investigate*
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- DG: maybe its an error pointing to a wrong calibration file?
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- On plots, don't supress -ve counts
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- Want to see where y=0 actually is, preferably by drawing a line there,
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then can clearly see what's y<0
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- SIMC rotation matrix differs from what Carlos has
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- Missing conversion from cartesian to spherical co-ords
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- Definition of what theta/phi for central spectrometer mean differ too
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- DG: Would it be easier to take output of SIMC and pass it through a
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converter/script to adjust the values
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- Copy what Carlos did and run this on the SIMC data
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- Some modifications needed
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- Should probably take values, convert them and save them to a new variable
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- Could just be added to repository as a standard tool
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- In Bill's LT-sep code, definitely seem to be missing a script still
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- Vijay noticed that there seems to be this missing link
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- Should be called "average_ratios.f", or something similar, which combines
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the different SHMS settings together to get full phi coverage
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- Average the ratios or sum the yields?
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- Either way should work, see notes from 2 weeks ago (23/01/19)
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Alicia Updates
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--------------
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BSA pi+n Analysis from KaonLT
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- Fixed dummy target subtraction with correct thickness factor
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- widened MM window and NPE threshold in SHMS Aerogel
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- Q2=3.0, W=2.32, 5 t-bin results
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- Asymmetry fits look a bit better now
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- Bin 2 (0.21<-t<0.29) still has a different phi-dependence than the rest
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- simple fit (A) vs full fit (A,B,C) differs by 2 sigma for Bin 2
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- The last t bin is very wide, please *remove* high t tail
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- comparison of preliminary LT' with VR Regge model
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- VR model has a known issue that is acknowledged in their paper
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- Does particularly bad at high -t (> 0.5)
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- VR curve does not extend to as low -t as the data
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- GH: this is because the curve is calculated with central kinematics only
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- need to compare VR to data at actual <Q2>,<W> for each t-bin
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- lowest -t bin will have a lower -t_min than the central kinematics, and
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the VR curve will then extend as low as the data
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- even with these issues, the VR comparo to data looks reasonable up to -t=0.5
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- Q2=3.0, W=2.32 AL data
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- asymmetry with dummy target data is consistent with zero to 1 sigma
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- Q2 = 4.4, W=2.74 first results
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- again see the second bin doing its own thing
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- difference between simple and full fits is only 1 sigma though
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- AL BSA is consistent with zero within errors
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- Q2 = 2.115 results
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- *need* finer t-binning, lots of stats
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- full and partial fits different by <1 sigma, bin 2 issue seems largely
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absent here
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- Looking at t-bin #2 more carefully
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- starting to get K+ leakthrough in bins 4,5. Bin 2 looks fairly clean
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- background between pi+N and K+Lambda peaks also grows in Bins 3,4,5
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- DG: Delta contribution seems to have a very different -t dependence to the
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neutron contribution, see a kink at MM=1.05
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- GH: piDelta has different t_min than pi+n, so that's why its absent in
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Bins 1,2
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- GH: wonders how big the pi+n radiative effects are for the higher t bins,
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and whether this explains the extra counts left of piDelta
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- we *need* to run SIMC for these settings and look at the growth of the
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MM radiative tail with t-bin to better understand this
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- will make a nice plot for the paper too
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- DG -For weird second tbin, have you looked at asymmetry before combining
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settings?
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- AP: Yes, overlayed, hard to interpret as statistics poorer
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- Nothing strange immediately jumping out
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- Can *try* at low Q2, where there are more stats, but the weird effect
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seems smaller there
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Jacob Updates
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new HMS saturation curve including higher momentum data
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- Saturation correction in B sets in above 5.1 GeV/c
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- shows 12% effect at P=6.8 GeV/c
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- DG: Isn't this removed in the magnet setting program?
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- checks, the program is unchanged since 2018-Aug-26
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- JM: using B/I from readback, so this is the real effect
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- Looking at Q1,Q2,Q3 saturation, expect to have more to show next week
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Nathan Updates
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--------------
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Detector time cuts update
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- Made an "open" cuts file
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- Wide enough that whole distribution can be seen
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- Summing over PMTs since the're stable
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- Doesn't change much between PMTs
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- Plots shown from run 13090, but other runs look the same
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- Dashed lines with suggested cuts
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- HMS Cherenkov looks odd
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- All events at zero for H.cer.goodAdcTdcDiffTime_PMT2
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- similarly variables for SHMS calorimeter all zero
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- GH: unfortunately, hcana initializes all variables to zero, instead of
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an error code of -9999, so it's not possible to distinguish a "true
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zero" from an "error code zero". Suspects this means the variable is
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actually not present, which is not the same as being present but zero
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- Maybe variable has been renamed to something else? *Investigate*
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- HMS Cherenkov distributions otherwise look fine
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- HMS Calorimeter double peaks are seen
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- most detectors have the right peak larger
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- some detectors have both peaks
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- others have left peak larger
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- making cut wide enough to include both peaks for now
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- GH: the bkd is down by 100X from the peak, so there is a bit more noise
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leaking in with wider cut, but probably okay
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- RT: yes, thinks so too
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Next Meeting
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------------
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Thur Feb 9 @ 17:00 Eastern/16:00 Regina/14:00 Pacific
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- PionLT will go first
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