Summary of observations
- As expected soft lepton B veto removes more LMx than ttbar
- again as expected the S/B ratio of LMx to SM is best at low lepton pT (less than 20 GeV ). Can this be somehow exploited?
- For some reason the mu-mu plots have a LMx peak for non-isolated muons. Understand!
Tables for ZVetos raw
We use 3 Modi of ZVetos. These are based on
- 1 hyp track and one non hyp track
- 2 non hyp tracks
- Modus 1. OR Modus 2.
Modus 1 is the most effective one. We will likely drop the other 2 variants eventually.
Modus 1
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
660.7 ± 10.1 |
109.6 ± 3.9 |
43.6 ± 2.2 |
94.2 ± 13.6 |
584.2 ± 23.8 |
818.8 ± 28.2 |
65.0 ± 8.3 |
7220.1 ± 56.4 |
649.5 ± 9.6 |
491.2 ± 13.3 |
43.3 ± 1.8 |
172.4 ± 5.7 |
10245.7 ± 70.8 |
mm |
150.2 ± 4.8 |
40.8 ± 2.4 |
19.7 ± 1.5 |
3.5 ± 2.0 |
0.0 ± 0.0 |
793.3 ± 27.7 |
10.5 ± 3.1 |
1951.6 ± 29.4 |
170.7 ± 4.9 |
230.1 ± 9.1 |
17.5 ± 1.1 |
67.8 ± 3.6 |
3140.2 ± 41.2 |
em |
410.5 ± 7.9 |
37.2 ± 2.3 |
5.5 ± 0.8 |
75.3 ± 12.0 |
0.0 ± 0.0 |
25.5 ± 5.7 |
49.6 ± 7.4 |
4100.6 ± 42.5 |
373.6 ± 7.3 |
94.8 ± 5.8 |
15.6 ± 1.1 |
59.3 ± 3.3 |
5077.8 ± 46.5 |
ee |
100.0 ± 3.9 |
31.7 ± 2.1 |
18.4 ± 1.4 |
15.5 ± 6.1 |
584.2 ± 23.8 |
0.0 ± 0.0 |
4.9 ± 2.0 |
1167.8 ± 22.6 |
105.3 ± 3.9 |
166.2 ± 7.7 |
10.1 ± 0.9 |
45.3 ± 2.9 |
2027.7 ± 34.0 |
Modus 1, 10%
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
6.8 ± 1.0 |
2.9 ± 0.6 |
1.3 ± 0.4 |
0.0 ± 0.0 |
64.1 ± 7.4 |
81.3 ± 8.2 |
8.1 ± 2.5 |
644.2 ± 17.2 |
4.8 ± 0.8 |
376.9 ± 11.7 |
33.7 ± 1.6 |
139.0 ± 5.1 |
813.5 ± 20.7 |
mm |
1.8 ± 0.5 |
1.7 ± 0.5 |
0.6 ± 0.3 |
0.0 ± 0.0 |
0.0 ± 0.0 |
81.3 ± 8.2 |
2.9 ± 1.5 |
184.9 ± 9.2 |
1.7 ± 0.5 |
179.2 ± 8.0 |
13.7 ± 1.0 |
56.1 ± 3.3 |
275.0 ± 12.5 |
em |
3.1 ± 0.7 |
0.7 ± 0.3 |
0.3 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
3.1 ± 1.6 |
352.6 ± 12.7 |
2.0 ± 0.5 |
71.4 ± 5.1 |
13.4 ± 1.0 |
48.0 ± 3.0 |
361.7 ± 12.9 |
ee |
1.8 ± 0.5 |
0.6 ± 0.3 |
0.4 ± 0.2 |
0.0 ± 0.0 |
64.1 ± 7.4 |
0.0 ± 0.0 |
2.0 ± 1.2 |
106.7 ± 7.0 |
1.1 ± 0.4 |
126.2 ± 6.7 |
6.7 ± 0.7 |
34.9 ± 2.6 |
176.8 ± 10.3 |
Modus 1, 1%
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
0.6 ± 0.3 |
0.1 ± 0.1 |
0.2 ± 0.2 |
0.0 ± 0.0 |
10.8 ± 3.1 |
10.7 ± 3.0 |
0.9 ± 0.9 |
51.4 ± 4.8 |
0.0 ± 0.0 |
132.0 ± 6.9 |
15.8 ± 1.1 |
58.0 ± 3.3 |
74.8 ± 6.5 |
mm |
0.2 ± 0.2 |
0.1 ± 0.1 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
10.7 ± 3.0 |
0.9 ± 0.9 |
19.0 ± 3.0 |
0.0 ± 0.0 |
64.9 ± 4.8 |
6.7 ± 0.7 |
25.7 ± 2.2 |
31.0 ± 4.4 |
em |
0.3 ± 0.2 |
0.0 ± 0.0 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
23.4 ± 3.2 |
0.0 ± 0.0 |
22.7 ± 2.9 |
5.7 ± 0.6 |
17.9 ± 1.8 |
23.8 ± 3.2 |
ee |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
10.8 ± 3.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
9.0 ± 2.0 |
0.0 ± 0.0 |
44.4 ± 4.0 |
3.3 ± 0.5 |
14.4 ± 1.6 |
20.0 ± 3.7 |
Modus 2
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
818.7 ± 11.2 |
230.4 ± 5.6 |
102.0 ± 3.4 |
110.9 ± 14.3 |
1324.5 ± 35.6 |
1942.2 ± 43.6 |
67.6 ± 8.5 |
9232.2 ± 63.8 |
819.1 ± 10.8 |
614.1 ± 14.9 |
57.7 ± 2.1 |
273.4 ± 7.2 |
14647.6 ± 88.3 |
mm |
181.1 ± 5.3 |
98.6 ± 3.7 |
50.3 ± 2.4 |
4.5 ± 2.3 |
0.0 ± 0.0 |
1913.4 ± 43.1 |
10.5 ± 3.1 |
2406.2 ± 32.6 |
208.3 ± 5.4 |
288.5 ± 10.2 |
23.2 ± 1.3 |
111.6 ± 4.6 |
4872.9 ± 54.9 |
em |
512.8 ± 8.9 |
61.6 ± 2.9 |
12.5 ± 1.2 |
87.9 ± 12.6 |
0.0 ± 0.0 |
28.8 ± 6.0 |
52.3 ± 7.6 |
5274.4 ± 48.2 |
474.3 ± 8.2 |
125.5 ± 6.7 |
20.6 ± 1.2 |
83.5 ± 4.0 |
6504.5 ± 52.3 |
ee |
124.9 ± 4.4 |
70.2 ± 3.1 |
39.3 ± 2.1 |
18.5 ± 6.3 |
1324.5 ± 35.6 |
0.0 ± 0.0 |
4.9 ± 2.0 |
1551.5 ± 26.0 |
136.5 ± 4.4 |
200.1 ± 8.5 |
13.9 ± 1.0 |
78.4 ± 3.8 |
3270.2 ± 45.2 |
Modus 2, 10%
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
10.4 ± 1.3 |
7.6 ± 1.0 |
3.6 ± 0.6 |
0.0 ± 0.0 |
139.7 ± 10.7 |
200.0 ± 12.9 |
8.7 ± 2.5 |
897.9 ± 20.3 |
6.6 ± 1.0 |
476.0 ± 13.1 |
45.6 ± 1.8 |
225.3 ± 6.5 |
1274.4 ± 26.5 |
mm |
3.7 ± 0.8 |
3.7 ± 0.7 |
2.1 ± 0.5 |
0.0 ± 0.0 |
0.0 ± 0.0 |
200.0 ± 12.9 |
2.9 ± 1.5 |
250.7 ± 10.7 |
2.1 ± 0.5 |
230.1 ± 9.1 |
17.8 ± 1.1 |
95.2 ± 4.2 |
465.2 ± 16.9 |
em |
4.6 ± 0.8 |
1.4 ± 0.4 |
0.4 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
3.7 ± 1.7 |
492.1 ± 15.0 |
2.8 ± 0.6 |
93.8 ± 5.8 |
18.1 ± 1.2 |
69.3 ± 3.6 |
505.1 ± 15.2 |
ee |
2.2 ± 0.6 |
2.5 ± 0.6 |
1.0 ± 0.3 |
0.0 ± 0.0 |
139.7 ± 10.7 |
0.0 ± 0.0 |
2.0 ± 1.2 |
155.1 ± 8.4 |
1.7 ± 0.5 |
152.2 ± 7.4 |
9.8 ± 0.9 |
60.8 ± 3.4 |
304.1 ± 13.7 |
Modus 2, 1%
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
1.5 ± 0.5 |
0.7 ± 0.3 |
0.7 ± 0.3 |
0.0 ± 0.0 |
18.3 ± 3.9 |
22.5 ± 4.4 |
0.9 ± 0.9 |
79.9 ± 6.0 |
0.0 ± 0.0 |
161.9 ± 7.6 |
21.0 ± 1.2 |
98.0 ± 4.3 |
124.6 ± 8.4 |
mm |
0.8 ± 0.3 |
0.4 ± 0.2 |
0.4 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
22.5 ± 4.4 |
0.9 ± 0.9 |
25.5 ± 3.4 |
0.0 ± 0.0 |
81.1 ± 5.4 |
8.4 ± 0.8 |
45.5 ± 2.9 |
50.5 ± 5.6 |
em |
0.6 ± 0.3 |
0.1 ± 0.1 |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
38.2 ± 4.1 |
0.0 ± 0.0 |
28.8 ± 3.2 |
8.4 ± 0.8 |
27.0 ± 2.3 |
39.2 ± 4.1 |
ee |
0.2 ± 0.2 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
18.3 ± 3.9 |
0.0 ± 0.0 |
0.0 ± 0.0 |
16.2 ± 2.7 |
0.0 ± 0.0 |
51.9 ± 4.3 |
4.2 ± 0.6 |
25.5 ± 2.2 |
34.8 ± 4.8 |
Modus 3
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
657.1 ± 10.0 |
108.0 ± 3.9 |
42.7 ± 2.2 |
94.2 ± 13.6 |
579.9 ± 23.7 |
813.8 ± 28.2 |
65.0 ± 8.3 |
7120.5 ± 56.0 |
643.9 ± 9.5 |
462.0 ± 12.9 |
40.5 ± 1.7 |
165.2 ± 5.6 |
10125.2 ± 70.4 |
mm |
149.7 ± 4.8 |
40.5 ± 2.4 |
19.5 ± 1.5 |
3.5 ± 2.0 |
0.0 ± 0.0 |
788.4 ± 27.6 |
10.5 ± 3.1 |
1934.1 ± 29.2 |
169.8 ± 4.9 |
218.2 ± 8.9 |
16.8 ± 1.1 |
65.5 ± 3.5 |
3116.0 ± 41.0 |
em |
409.0 ± 7.9 |
36.6 ± 2.2 |
5.3 ± 0.8 |
75.3 ± 12.0 |
0.0 ± 0.0 |
25.5 ± 5.7 |
49.6 ± 7.4 |
4047.8 ± 42.2 |
371.3 ± 7.2 |
90.2 ± 5.7 |
14.5 ± 1.0 |
56.6 ± 3.3 |
5020.4 ± 46.2 |
ee |
98.4 ± 3.9 |
30.9 ± 2.1 |
18.0 ± 1.4 |
15.5 ± 6.1 |
579.9 ± 23.7 |
0.0 ± 0.0 |
4.9 ± 2.0 |
1138.6 ± 22.3 |
102.7 ± 3.8 |
153.6 ± 7.4 |
9.2 ± 0.8 |
43.1 ± 2.9 |
1988.9 ± 33.7 |
Modus 3, 10%
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
6.6 ± 1.0 |
2.8 ± 0.6 |
1.3 ± 0.4 |
0.0 ± 0.0 |
63.4 ± 7.4 |
78.7 ± 8.1 |
8.1 ± 2.5 |
613.7 ± 16.8 |
4.7 ± 0.8 |
350.2 ± 11.2 |
31.1 ± 1.5 |
132.4 ± 5.0 |
779.1 ± 20.2 |
mm |
1.8 ± 0.5 |
1.5 ± 0.5 |
0.6 ± 0.3 |
0.0 ± 0.0 |
0.0 ± 0.0 |
78.7 ± 8.1 |
2.9 ± 1.5 |
175.8 ± 9.0 |
1.7 ± 0.5 |
168.1 ± 7.8 |
13.0 ± 1.0 |
53.8 ± 3.2 |
263.0 ± 12.2 |
em |
2.9 ± 0.7 |
0.7 ± 0.3 |
0.3 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
3.1 ± 1.6 |
337.2 ± 12.4 |
1.8 ± 0.5 |
67.4 ± 4.9 |
12.4 ± 1.0 |
45.5 ± 2.9 |
346.0 ± 12.6 |
ee |
1.8 ± 0.5 |
0.6 ± 0.3 |
0.4 ± 0.2 |
0.0 ± 0.0 |
63.4 ± 7.4 |
0.0 ± 0.0 |
2.0 ± 1.2 |
100.7 ± 6.8 |
1.1 ± 0.4 |
114.7 ± 6.4 |
5.8 ± 0.7 |
33.0 ± 2.5 |
170.1 ± 10.1 |
Modus 3, 1%
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
0.6 ± 0.3 |
0.1 ± 0.1 |
0.2 ± 0.2 |
0.0 ± 0.0 |
10.8 ± 3.1 |
9.7 ± 2.9 |
0.9 ± 0.9 |
47.7 ± 4.6 |
0.0 ± 0.0 |
121.2 ± 6.6 |
14.1 ± 1.0 |
54.9 ± 3.2 |
70.1 ± 6.3 |
mm |
0.2 ± 0.2 |
0.1 ± 0.1 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
9.7 ± 2.9 |
0.9 ± 0.9 |
17.2 ± 2.8 |
0.0 ± 0.0 |
59.1 ± 4.6 |
6.2 ± 0.7 |
24.4 ± 2.1 |
28.2 ± 4.1 |
em |
0.3 ± 0.2 |
0.0 ± 0.0 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
21.5 ± 3.0 |
0.0 ± 0.0 |
21.6 ± 2.8 |
5.0 ± 0.6 |
17.2 ± 1.8 |
22.0 ± 3.1 |
ee |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
10.8 ± 3.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
9.0 ± 2.0 |
0.0 ± 0.0 |
40.4 ± 3.8 |
2.9 ± 0.5 |
13.4 ± 1.6 |
20.0 ± 3.7 |
Determine cuts for 10% and 1% of background efficiency using scalar SumEt as cut
10% cuts
Using electron veto for just used for
SumEt
We will use a cut at
SumEt > 225
GeV for the 10% cuts for the time being (081113).
Full tables below.
Table below is for 225
GeV :
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
total |
all |
11.7 ± 1.3 |
1.4 ± 0.4 |
0.7 ± 0.3 |
0.0 ± 0.0 |
10.3 ± 2.9 |
39.6 ± 5.8 |
7.3 ± 2.4 |
773.8 ± 18.8 |
6.6 ± 1.0 |
401.0 ± 12.0 |
29.9 ± 1.5 |
97.8 ± 4.3 |
1380.1 ± 23.9 |
mm |
3.8 ± 0.8 |
0.7 ± 0.3 |
0.4 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
39.6 ± 5.8 |
2.2 ± 1.3 |
197.0 ± 9.5 |
2.1 ± 0.5 |
202.3 ± 8.5 |
11.4 ± 0.9 |
27.8 ± 2.3 |
487.4 ± 14.4 |
em |
5.5 ± 0.9 |
0.6 ± 0.3 |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
3.8 ± 1.7 |
468.7 ± 14.7 |
3.1 ± 0.7 |
64.2 ± 4.8 |
13.2 ± 1.0 |
52.7 ± 3.2 |
612.0 ± 15.9 |
ee |
2.3 ± 0.6 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
10.3 ± 2.9 |
0.0 ± 0.0 |
1.3 ± 0.9 |
108.0 ± 7.0 |
1.4 ± 0.4 |
134.5 ± 7.0 |
5.3 ± 0.6 |
17.4 ± 1.8 |
280.6 ± 10.5 |
Table below is for 200
GeV :
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
total |
all |
16.3 ± 1.6 |
1.5 ± 0.5 |
0.8 ± 0.3 |
0.0 ± 0.0 |
14.3 ± 3.5 |
45.8 ± 6.3 |
8.3 ± 2.6 |
1002.4 ± 21.4 |
12.4 ± 1.3 |
416.9 ± 12.3 |
30.5 ± 1.5 |
101.4 ± 4.4 |
1650.5 ± 26.4 |
mm |
5.1 ± 0.9 |
0.8 ± 0.3 |
0.4 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
45.8 ± 6.3 |
3.2 ± 1.6 |
257.3 ± 10.9 |
4.4 ± 0.8 |
211.0 ± 8.7 |
11.6 ± 0.9 |
28.1 ± 2.3 |
567.7 ± 15.6 |
em |
8.6 ± 1.1 |
0.6 ± 0.3 |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
3.8 ± 1.7 |
598.1 ± 16.6 |
5.7 ± 0.9 |
67.4 ± 4.9 |
13.2 ± 1.0 |
54.6 ± 3.2 |
752.2 ± 17.8 |
ee |
2.6 ± 0.6 |
0.1 ± 0.1 |
0.1 ± 0.1 |
0.0 ± 0.0 |
14.3 ± 3.5 |
0.0 ± 0.0 |
1.3 ± 0.9 |
146.9 ± 8.2 |
2.4 ± 0.6 |
138.5 ± 7.1 |
5.6 ± 0.6 |
18.7 ± 1.9 |
330.6 ± 11.6 |
1% cuts
Using electron veto for just used for
SumEt
We will use a cut at
SumEt > 525
GeV for the 1% cuts for the time being (081113).
Full tables below.
Table below is for 525
GeV :
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
SM total |
all |
1.7 ± 0.5 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
2.6 ± 1.5 |
6.8 ± 2.4 |
0.9 ± 0.9 |
79.5 ± 5.9 |
0.0 ± 0.0 |
142.4 ± 7.2 |
14.2 ± 1.0 |
39.8 ± 2.7 |
91.6 ± 6.7 |
mm |
0.6 ± 0.3 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
6.8 ± 2.4 |
0.9 ± 0.9 |
22.8 ± 3.2 |
0.0 ± 0.0 |
77.5 ± 5.3 |
5.2 ± 0.6 |
10.2 ± 1.4 |
31.1 ± 4.1 |
em |
0.9 ± 0.4 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
41.6 ± 4.3 |
0.0 ± 0.0 |
18.8 ± 2.6 |
6.7 ± 0.7 |
22.1 ± 2.0 |
42.6 ± 4.3 |
ee |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
2.6 ± 1.5 |
0.0 ± 0.0 |
0.0 ± 0.0 |
15.1 ± 2.5 |
0.0 ± 0.0 |
46.2 ± 4.1 |
2.4 ± 0.4 |
7.6 ± 1.2 |
17.9 ± 3.0 |
Table below is for 550
GeV :
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
total |
all |
1.4 ± 0.5 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
2.0 ± 1.4 |
6.8 ± 2.4 |
0.9 ± 0.9 |
66.1 ± 5.4 |
0.0 ± 0.0 |
131.6 ± 6.9 |
13.7 ± 1.0 |
36.4 ± 2.6 |
259.1 ± 9.7 |
mm |
0.6 ± 0.3 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
6.8 ± 2.4 |
0.9 ± 0.9 |
17.8 ± 2.8 |
0.0 ± 0.0 |
71.8 ± 5.1 |
5.1 ± 0.6 |
9.3 ± 1.3 |
112.2 ± 6.5 |
em |
0.6 ± 0.3 |
0.1 ± 0.1 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
35.0 ± 3.9 |
0.0 ± 0.0 |
16.6 ± 2.4 |
6.4 ± 0.7 |
20.8 ± 2.0 |
79.5 ± 5.1 |
ee |
0.2 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
2.0 ± 1.4 |
0.0 ± 0.0 |
0.0 ± 0.0 |
13.3 ± 2.4 |
0.0 ± 0.0 |
43.3 ± 4.0 |
2.1 ± 0.4 |
6.4 ± 1.1 |
67.3 ± 5.0 |
Table below is for 600
GeV :
|
ww |
wz |
zz |
wjets |
dyee |
dymm |
dytt |
ttbar |
tw |
LM1 |
LM2 |
LM4 |
total |
all |
0.6 ± 0.3 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
2.0 ± 1.4 |
5.4 ± 2.2 |
0.9 ± 0.9 |
46.2 ± 4.5 |
0.0 ± 0.0 |
101.0 ± 6.0 |
11.2 ± 0.9 |
30.2 ± 2.4 |
197.5 ± 8.4 |
mm |
0.3 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
5.4 ± 2.2 |
0.9 ± 0.9 |
11.2 ± 2.2 |
0.0 ± 0.0 |
55.5 ± 4.5 |
4.1 ± 0.5 |
8.3 ± 1.3 |
85.7 ± 5.7 |
em |
0.3 ± 0.2 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
25.0 ± 3.3 |
0.0 ± 0.0 |
11.9 ± 2.1 |
5.4 ± 0.6 |
16.6 ± 1.8 |
59.2 ± 4.3 |
ee |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
0.0 ± 0.0 |
2.0 ± 1.4 |
0.0 ± 0.0 |
0.0 ± 0.0 |
10.0 ± 2.1 |
0.0 ± 0.0 |
33.5 ± 3.5 |
1.7 ± 0.4 |
5.3 ± 1.0 |
52.5 ± 4.4 |
--
IngoBloch - 12 Nov 2008
Topic revision: r5 - 17 Nov 2008 - 17:38:04 -
IngoBloch