DiscoveringHeavyParticles
Introduction
This note demonstrates a recently proposed method for determining the mass of boosted particles from their decay products by exploiting the substructure of the resulting single collimated jet using the kT algorithm. We illustrate this method with a simple RPV SUSY model using the ATLAS detector at the LHC. We consider the hadronic decay of boosted neutralinos into single jets composed of three collimated subjets. We consider up to 1fb-1 of integrated luminosity with 10TeV simulated data.
The ATL-PHYS-PUB-2009-076 note can be found
here
Pseudo cone-radius as a function of neutralino pT
pT vs. mass for jets in events with at least four jets with |eta| < 2.5 for 1 fb−1
Jet mass for jets with pT > 275GeV in events with at least four jets with |eta| < 2.5
y2 vs. y1 for jets with pT >275GeV in events with at least four jets with |h|<2.5 (distributions
normalised to unity)
Jet mass for jets with pT > 275GeV and y2 > −0.17y1 +0.08 in events passing all event
selection cuts
Jet pT for jets with pT > 275GeV and y2 > −0.17y1+0.08 in signal events passing all event
selection cuts
Jet mass for jets with pT > 275
GeV and y2 > −0.17y1 +0.08 in events passing all event
selection cuts
|
Cut 1 |
Cuts 1 & 2 |
Cuts 1,2 & 3 |
Cuts 1,2,3 & 4 |
SUSY |
14577 |
5849 |
792 |
347 |
t ¯t |
2.3×10^5 |
2,000 |
200 |
1 |
dijets |
3.2×10^9 |
1.1×10^6 |
1.8×10^4 |
1100 |
W+jets |
1500 |
20 |
20 |
0 |
Z+jets |
1.9×10^4 |
210 |
2 |
1 |
Table 2: Offline Cut Flow (all counts are Events per 1 fb−1)
Trigger Name |
Total |
Prescale Effic. before event selection (%) |
Effic. after event selection (%) |
J350 |
1 |
50.0 |
82.7 |
3J180 |
1 |
56.0 |
98.3 |
4J95 |
20 |
77.6 |
99.6 |
3J60 |
1000 |
95.0 |
99.6 |
J265 |
15 |
75.5 |
99.6 |
4J125 |
1 |
55.8 |
99.6 |
JE280 |
2 |
91.0 |
100 |
JE340 |
1 |
83.2 |
100 |
Table 3: Trigger efficiencies for various jet triggers on RPV SUSY events.