1
|
Oct 10/25 PionLT/KaonLT Analysis Meeting Notes
|
2
|
----------------------------------------------
|
3
|
(Notes by GH)
|
4
|
|
5
|
Today: KaonLT 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, Alicia Postuma, Nathan Heinrich, Nermin Sadoun,
|
13
|
Vijay Kumar, Nacer Hamdi, Muhammad Junaid
|
14
|
FIU - Pete Markowitz
|
15
|
CUA - Chi Kin Tam, BC Manoj, Tanja Horn, Sameer Jain
|
16
|
Virginia - Richard Trotta
|
17
|
Ohio - Julie Roche
|
18
|
CSULA - Konrad Aniol
|
19
|
JMU - Ioana Niculescu, Gabriel Niculescu
|
20
|
|
21
|
Vijay
|
22
|
-----
|
23
|
Summer 2019 PionLT data analysis
|
24
|
- CoinBlocking correction
|
25
|
- made plots of CTime.CoinTime_RAW_ROC1,2
|
26
|
- ROC1 plot is cleaner than ROC2, will use this one
|
27
|
- found oscilloscope traces of trigger timing at logentry #3655655
|
28
|
- based on oscilloscope tracs, the timing cut window should be ~140ns wide
|
29
|
|
30
|
- pion absoprtion correction
|
31
|
- will apply correction previously determined with Alicia's Geant4 simulation
|
32
|
|
33
|
Sameer
|
34
|
------
|
35
|
KaonLT high Q2 CoinBlocking correction
|
36
|
- looking at Q2=2.115 data taken on 2018.10.02
|
37
|
|
38
|
Chi Kin
|
39
|
-------
|
40
|
KaonLT Q2=3.0, W=3.14 data analysis
|
41
|
- MissingMass checks
|
42
|
- applying cut 1.10<MM<1.14 to select K+Lambda region for both data and MC
|
43
|
- pion subtraction applied to data
|
44
|
- previous error needing large MM shift to data was fixed, the shift is only
|
45
|
a few MeV now. However, correcting both data and MC, as neither are at PDG
|
46
|
mass
|
47
|
- *NB* Tanja: you need to remove the MM shift from the MC, the Lambda peak
|
48
|
will be at a mass slightly higher than PDG value due to energy loss in
|
49
|
the target and other materials. Just shift the data to the MC peak
|
50
|
position
|
51
|
|
52
|
- Data & SIMC plot comparisons
|
53
|
- various differences in the distributions, particularly for right SHMS
|
54
|
setting
|
55
|
- Gabriel: pion leakthrough subtraction has a different delta-distribution
|
56
|
than K+Lambda data, how do you correct for this?
|
57
|
- Richard: shows Q2=4.4 pion subtraction
|
58
|
- needs to add an empirical fit underneath the Lambda, Sigma peaks that
|
59
|
is not removed by the pion leakthrough subtraction
|
60
|
- RF timing information was added mid-way through Q2=3.0, W=3.14 setting.
|
61
|
The Q2=5.5 setting has it, so these data have much less pion
|
62
|
leakthrough than the other settings.
|
63
|
- Tanja: Chi Kin is intentionally treating the background different than
|
64
|
Richard, so we can better understand how reproducible the results are
|
65
|
|
66
|
- LT-sep iterations with 10 phi-bins
|
67
|
- after 4 iterations, Data/MC ratios are much closer to unity
|
68
|
- L/T/LT/TT functional forms are the same as Richard's, but parameters are
|
69
|
different
|
70
|
- separated cross section ratios are fairly stable from IT=0,4,8
|
71
|
- Julie: the Data/MC ratios have phi-dependence, but the sig_uns are flatter.
|
72
|
Does this mean the model has a larger (and wrong) phi-dependence compared
|
73
|
to the data?
|
74
|
- Tanja, Garth: yes this is what it means. The LT/TT cross sections are
|
75
|
determined directly from the Rosenbluth fits of sig_uns. It will be
|
76
|
important to confirm the model dependence in the result is small.
|
77
|
|
78
|
Alicia
|
79
|
------
|
80
|
Difficulties re-submitting the pi+n BSA paper to PhysLettB
|
81
|
- editorial manager portal has changed completely since initial submission
|
82
|
- need to upload XML info for all authors via undefined "standard procedure"
|
83
|
- no guidelines given, following INSPIRE-HEP instructions for now
|
84
|
- using ror.org Research Organization Registration for institution
|
85
|
addresses, which is helpful
|
86
|
- need to include ORCiD numbers for all authors included in MetaData. Did a
|
87
|
lot of work to find ORCiD for most people, but a few have left the field and
|
88
|
don't have one
|
89
|
- Tanja: please contact Haiyan Gao directly, including screenshots of where
|
90
|
you're encountering problems
|
91
|
|
92
|
Richard
|
93
|
-------
|
94
|
Computer Physics Communications paper on LT-function fitting algorithm
|
95
|
- combined Fpi-2 data for both Q2=1.6, 2.45 into one dataset (t-dep only) and
|
96
|
put it through the fitting algorithm
|
97
|
- algorithm improves the Chi-squared compared to earlier results
|
98
|
- got CSV files from Vijay(pi+n) and Nacer(K+L) on their separated
|
99
|
low Q2 cross-sections
|
100
|
- next step will be to include these in the fits
|
101
|
|
102
|
Q2=4.4 LT-separations
|
103
|
- data has pion subtraction and empirical fit underneath Lambda
|
104
|
- no Sigma fit is included
|
105
|
- equations slightly different than what Chi Kin is using
|
106
|
- Data & SIMC plot comparisons
|
107
|
- center SHMS setting, SIMC has narrower Q2,W-distributions than data
|
108
|
- acceptance plots look good for both SHMS settings
|
109
|
- Data/MC ratios between 0.75 and 1.5
|
110
|
- surprisingly, the lower -t bins have worse ratios than high -t bins
|
111
|
- might be a pion leakage issue at low -t, Richard will have to look into
|
112
|
it
|
113
|
- *NB* Tanja: please make a comparison of Richard and Chi Kin's
|
114
|
background subtractions for this setting
|
115
|
- made a weighted verage of phi-bins at each epsilon similar to what Vijay
|
116
|
showed last week
|
117
|
- it shows that high epsilon>low epsilon, which is good news
|
118
|
- sigL<<sigT for all bins
|
119
|
- Garth and Tanja willing to compare separated results with VGL model when
|
120
|
things are ready
|
121
|
|
122
|
Nacer
|
123
|
-----
|
124
|
KaonLT Q2=0.50 LT-separations
|
125
|
- rechecking Data & SIMC MM distributions to be sure pion leakthrough is not an
|
126
|
issue
|
127
|
- to recap, sigL has a surprisingly large peak at low -t that is suspicious
|
128
|
- RF timing cut is available for these data, so pion contamination is small
|
129
|
- Data/MC ratios are fairly flat 0.8-1.2 at low epsilon, some phi-oscillations
|
130
|
at high epsilon, particularly for higher -t bins
|
131
|
- shows MM plots for 7 t-bins for center SHMS low epsilon, then shows for
|
132
|
t-phi bins (i.e. dividing each t-bin into phi bins)
|
133
|
- pion subtraction looks very good, no evidence that background is the
|
134
|
cause of the weird sigL at low -t
|
135
|
- *NB* Garth: SIMC normalization seems off for t-phi bins, compared to
|
136
|
t-bins, plotting script needs to be rechecked
|
137
|
|
138
|
- will go back to model optimization
|
139
|
- had LT=TT=0 functional forms in model
|
140
|
- earlier, had tried Fpi-2 parameterization, but this gave bad ratios, so
|
141
|
stopped
|
142
|
- then tried changing LT,TT functional forms to same as L,T forms in
|
143
|
sig_factorized_2007. This looks more promising, so will do more iterations
|
144
|
|
145
|
Nathan
|
146
|
------
|
147
|
PionLT Coin Lumi analysis
|
148
|
- calculating systematic uncertainties on Coin Blocking correction
|
149
|
- will move timing cuts by 5 ns in and out
|
150
|
- *NB* Vijay: suggest to take 1 beam bucket (4ns) left and right instead
|
151
|
- will take symmetric cuts around main distribution for systematic
|
152
|
uncertainties
|
153
|
- Garth: unless there is a good reason for asymmetric cuts in the error
|
154
|
analysis, suggest to keep the cuts as symmetric
|
155
|
|
156
|
- calculating LiveTime systematic errors
|
157
|
- compared CPU*ELLT to EDTM values
|
158
|
- the difference gave a ~4% difference at high coin rate, which is
|
159
|
suspiciously similar to the AdHoc correction discussed earlier
|
160
|
- Garth had suggested to recalculate the normalized coin yields (after Coin
|
161
|
Blocking) with EDTM instead of CPU*ELLT
|
162
|
** the resulting distribution is flat, which means no AdHoc correction
|
163
|
** would be needed
|
164
|
- clearly this means the EDTM is capturing some element of deadtime that
|
165
|
CPU*ELLT misses
|
166
|
** will use EDTM for all coin data, and no AdHoc correction!
|
167
|
- EDTM is still unreliable for singled data though
|
168
|
- will need to evaluate a systematic uncertainty in the EDTM
|
169
|
- suggests to fit each TLT vs Rate for each CoinLumi setting and look at the
|
170
|
spread of points from the fit curve
|
171
|
- concerned that simply combining the variations between the settings, as the
|
172
|
TLT differences them (at same CoinRate) are probably real
|
173
|
- *NB* Gabriel: suggests to make a histogram of the residuals between the
|
174
|
data and fit function and see if this gives a Gaussian distribution
|
175
|
- *NB* Julie: the used logarithmic fit diverges at zero rate. It's important
|
176
|
to switch to an exponential fit that goes to 1 at zero rate
|
177
|
|
178
|
Junaid
|
179
|
------
|
180
|
PionLT Q2=3.85 LT-separations
|
181
|
- working on LT,TT functional forms to reduce oscillations in Data/MC ratios
|
182
|
- ratios are 0.8 to 1.2, but with 2-bump oscillations coming from TT
|
183
|
- Rosenbluth fits give sigL>sigT at low -t and fairly small LT,TT
|
184
|
- will need to modify the sigTT functional form
|
185
|
- sigLT functional form seems fine, based on much smaller 1-bump oscillation
|
186
|
in ratios
|
187
|
|
188
|
Nermin
|
189
|
------
|
190
|
PionLT data analysis
|
191
|
- met w/ Junaid on hcana software setup
|
192
|
- reading up on Hall C detector systems
|
193
|
|
194
|
Next Meeting
|
195
|
------------
|
196
|
We will try our new 2-meeting/week structure
|
197
|
- Thurs: Oct 16 @ 16:00 Eastern/14:00 Regina
|
198
|
- PionLT will go first
|
199
|
- Fri: Oct 17 @ 11:00 Eastern/9:00 Regina
|
200
|
- KaonLT will go first
|
201
|
|
202
|
|
203
|
|
204
|
|
205
|
|
206
|
|
207
|
|
208
|
|
209
|
|