Download presentation
Presentation is loading. Please wait.
Published byTravis Surgent Modified over 10 years ago
1
Jet energy correction (Zmumu, 10k) June 4,2008 Jongseok Lee (Sungkyunkwan University) 1
2
# of jet 2 red : calojet green : genjet pt>15, ΔR(jet,mu)>0.5
3
Jet energy correction factor 3 P T (calojet) factor
4
Matching jet with MC μ 4 Δ R(genjet,mcmu) P T (genjet)/P T (mcmu) Δ R(corjet,mcmu) P T (corjet)/P T (mcmu) Δ R(genjet,mcmu) Δ R(corjet,mcmu) P T (genjet)/P T (mcmu)P T (corjet)/P T (mcmu) no cut pt>15
5
nConstituent 5 no corrected nC pt>15 no corrected nC pt>15 ΔR(jet,mcmu)>0.5 red : corjet, black : genjet corrected nC pt>15 corrected nC pt>15 ΔR(jet,mcmu)>0.5
6
Average P T of jet tower 6 corrected nC pt>15 corrected nC pt>15 ΔR(jet,mcmu)>0.5 red : corjet, black : genjet
7
# of jet 7 pt>15, ΔR(jet,mu)>0.5 pt>15 pt>15, nC>=5, ΔR(jet,mu)>0.5 pt>15, nC>=5 red : corjet, black : genjet
8
PTPT 8 pt>15, ΔR(jet,mu)>0.5 pt>15 pt>15, nC>=5, ΔR(jet,mu)>0.5 pt>15, nC>=5
9
η 9 red : corjet, black : genjet pt>15, ΔR(jet,mu)>0.5 pt>15 pt>15, nC>=5, ΔR(jet,mu)>0.5 pt>15, nC>=5
10
Jet efficiency (corjet/genjet) 10 pt>15, ΔR(jet,mu)>0.5 pt>15 black : pt>15, ΔR(jet,mu)>0.5 red : pt>15 black : pt>15, ΔR(jet,mu)>0.5 red : pt>15
11
back up 11
12
Jet energy correction factor 12 Many reasons why a calorimeter jet energy differs from an underlying particle and parton jet energies: Energy offset due to electronics noise and event pile-up Energy lost due to energy thresholds applied at cell and tower level Energy lost due to particles bent away in 4T magnetic field Nonlinear HCAL response (e/h < 1)
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.