1
|
Feb 8/24 PionLT/KaonLT Analysis Meeting Notes
|
2
|
---------------------------------------------
|
3
|
(Notes by GH)
|
4
|
|
5
|
Today: PionLT will be discussed first
|
6
|
|
7
|
Please remember to post your slides at:
|
8
|
https://redmine.jlab.org/projects/kltexp/wiki/Kaon_LT_Meetings
|
9
|
|
10
|
Present
|
11
|
-------
|
12
|
Regina - Garth Huber, Ali Usman, Muhammad Junaid, Nacer Hamdi
|
13
|
CSULA - Konrad Aniol
|
14
|
York - Stephen Kay
|
15
|
JLab - Dave Gaskell
|
16
|
CUA - Richard Trotta, Tanja Horn
|
17
|
|
18
|
Junaid
|
19
|
------
|
20
|
Errors on Tracking Efficiencies for Heep singles data
|
21
|
- found the error in the calculation
|
22
|
- data is replayed, will be looking at the results soon
|
23
|
|
24
|
Richard
|
25
|
-------
|
26
|
SIMC Weights
|
27
|
- last week's issue was due to weight not being applied to SIMC yields
|
28
|
- with this fixed, the 10^6 factor is no longer needed
|
29
|
- now getting Data/MC ratios of 0.2-0.5
|
30
|
|
31
|
SIMC Missing Mass
|
32
|
- last week reported a very long K+Lambda radiative tail, the opposite that was
|
33
|
found for the pi+ analysis
|
34
|
- Dave looked at RT's input files, and found that the wrong K+ decay length was
|
35
|
used
|
36
|
- 780.4cm was used instead of 371.2cm (i.e. pi+ value instead of K+ value)
|
37
|
- SIMC would have generated the correct K+ decay products, but with the wrong
|
38
|
probablity
|
39
|
- the fact that the user has to input the correct decay length (instead of it
|
40
|
being selected automatically since SIMC already knows it's handling K+
|
41
|
decay) is a historic artifact from Dave Koltenuk days
|
42
|
- a second issue was that MM was not recalculated for SIMC events by the
|
43
|
recon_hcana_script
|
44
|
- with these corrected, the K+ radiative tail agrees better with the data, of
|
45
|
course the data are still subject to change as well, until the PID cut study
|
46
|
is completed
|
47
|
|
48
|
K+ PID Studies
|
49
|
- investigating pi+ and proton leakthrough into K+ sample
|
50
|
- selected three different MM regions:
|
51
|
MM<1.05 (should be mostly leakthrough protons)
|
52
|
MM>1.16 (will contain leakthrough pi+ as well as real K+)
|
53
|
K+Lambda region is 1.06<MM<1.16
|
54
|
- for MM<1.05 region, look at Aerogel NPE distribution
|
55
|
- saw some evidence of proton leakthrough
|
56
|
- tightened cut
|
57
|
before: events with >3NPE accepted
|
58
|
now: events with >4.5NPE accepted
|
59
|
- still need to adjust HGC hole cut
|
60
|
- HGC optics were adjusted between low and high epsilon runs, need larger
|
61
|
hole cut for 10.6 GeV data
|
62
|
- MM>1.16 region, again look at Aerogel
|
63
|
- will try 4.5NPE cut, maybe need 4NPE if cut is too restrictive
|
64
|
- need to apply same Aerogel cut to all MM regions
|
65
|
|
66
|
Data/MC Yield Comparisons
|
67
|
- looking at Q2=2.115 yields with different MM cuts
|
68
|
- ratios are closer to 1 with 1.06<MM<1.16 cut applied
|
69
|
|
70
|
Separated Xsect Comparisons
|
71
|
- iteration scripts seem to work
|
72
|
- some discussion of what units used for cross-sections in SIMC, Richard still
|
73
|
doing final checks
|
74
|
|
75
|
Next Steps
|
76
|
- finish PID studies
|
77
|
- finish cut analysis
|
78
|
|
79
|
Ali
|
80
|
---
|
81
|
Compare pi+n MM dists of Data and SIMC with Dave's delta fix
|
82
|
- Bad News: somehow the Data MM distributions before and after delta fix are
|
83
|
identical, which is suspicious. Will discuss w/Alicia after she's back
|
84
|
- Plots for Q2=5 are shown, others behave the same way
|
85
|
- Good News: adjusted Drift Chamber resolution parameter in SIMC
|
86
|
- with the adjustment, the pi+MM peak agreement between Data and SIMC is
|
87
|
significantly better
|
88
|
- only adjusted the SHMS resolution so far, since it's higher rate
|
89
|
- HMS routine already had some resolution tuning (apparently from Doug
|
90
|
Koltenuk), while SHMS lacks this code
|
91
|
- Dave: Abideh will look at HMS inclusive data and tweak HMS resolution there.
|
92
|
He can provide his HMS parameters when he's done, so the effects of the two
|
93
|
spectrometers can be separated that way
|
94
|
- Dave: the DC intrinsic resolution should not be strongly rate dependent.
|
95
|
However, at higher rates, the Gaussian tail fraction does increase.
|
96
|
- Koltenuk's HMS resolution tuning is along this idea, with a double Gaussian
|
97
|
distribution giving bigger tails
|
98
|
- Dave: when comparing SIMC to Data MM distribution, try to confine your study
|
99
|
to the region just around the pi+ peak, to avoid attributing DC resolution
|
100
|
issues to what might be problems in the treatment of the radiative tail
|
101
|
- suggest to look at +/-2 sigma region around pi+ peak, so MM<0.98
|
102
|
- really hoping the SHMS DC resolution parameter does not turn out to be
|
103
|
kinematics dependent. If so, this would indicate that other parts of the
|
104
|
simulation (such as multiple scattering) are incomplete
|
105
|
|
106
|
Nacer
|
107
|
-----
|
108
|
KaonLT low Q2 DC calibs 95% done
|
109
|
- submitted last jobs this morning
|
110
|
|
111
|
Next Steps
|
112
|
- will need to replay all data with new DC calibs, and offsets
|
113
|
- then can start looking at K+ PID
|
114
|
- Note: Aerogel index (n) will be higher than in Richard's data
|
115
|
|
116
|
Stephen
|
117
|
-------
|
118
|
Notes that starting a new WorkFlow on SWIF seems to give a better success rate
|
119
|
on iFarm jobs
|
120
|
- Nacer notices the same effect
|
121
|
|
122
|
Next Meeting
|
123
|
------------
|
124
|
- Thur Feb 15 @ 15:00 Eastern/14:00 Regina
|
125
|
- KaonLT will go first
|
126
|
|
127
|
|