CMS Data Analysis Patrick Mooney Trinity School South Bend, IN Jill Ziegler Hamilton High West Hamilton, NJ Megan Gillian La Lumiere School LaPorte, IN Nick Schrock Bethany Christian Schools Goshen, IN
Starting Points Work last summer with the tt̅ single muon data set and tutorial by Drs. Sander and Schmidt – dimuon mass – preliminary work viewing plots – preliminary estimation of cuts for top events Foundational work with C and C++
Data Updates and Access Data set, Monte Carlo background simulations, and Tutorial updated in fall 2014 by Drs. Sander and Schmidt – Added three new background simulation types New tutorial data and sample programs uploaded to server by Dr. Dan Karmgard – Access to server through virtual terminal – Individual directory space for each user Library created for shared unmodified files by Dr. Karmgard – Holds archive copies of frequently modified files – Holds working library of infrequently modified files – Main program files modified to call data directly from central library
Histogram Plotting Works through subprogram “Plotter” Data or simulated tt̅ plotted as points Simulated background stacked Changes to stock programs – Color changes to background for clarity – Option for non-log plots added – Color legend moved to make room for histogram data legend
tt̅ Mass Plot One goal of tutorial is finding the mass of the top quark from tt̅ events – Examining decay mode producing four jets (including two jets from b quarks), a single lepton (muon), and a neutrino
tt̅ Events
tt̅ Mass Plot One goal of tutorial is finding the mass of the top quark from tt̅ events – Examining decay mode producing four jets (including two jets from b quarks), a single lepton (muon), and a neutrino Two ways to calculate: – Two jets from W decay plus b jet – Muon and neutrino from W decay plus b jet
Refining Plots with tt̅ Simulation Treated tt̅ simulated data like data in histograms – unstacked point Created histograms to see – what tt̅ plots should look like – how other data differed
Refining Plots with tt̅ Simulation (cont.) Focused on histograms of – number of jets – number of jets from b quarks – transverse momentum of jets – missing transverse energy (from neutrino) – cosine of muon angle from beamline – mass of W boson decaying to two jets Made trial cuts to see – how many events were cut – how cuts changed background vs. tt̅
Interesting Preliminary Note Histograms of data with no cuts show W mass and t mass at approximately correct places (W ≈ 80 GeV, t ≈ 173 GeV)
Refining Plots with tt̅ Simulation (cont.) Cuts specific to W to 2 jets plus b jet: – Require at least 4 jets: at least 2 b jets at least 2 non-b jets
Refining Plots with tt̅ Simulation (cont.) Cuts specific to W to 2 jets plus b jet : – Require at least 4 jets: at least 2 b jets at least 2 non-b jets
Refining Plots with tt̅ Simulation (cont.) Cuts specific to W to 2 jets plus b jet : – Require mass of W decaying to 2 jets to be within reasonable range (greater than 60 GeV, less than 110 GeV)
Refining Plots with tt̅ Simulation (cont.) Cuts specific to W to 2 jets plus b jet : – Require mass of W decaying to 2 jets to be within reasonable range (greater than 60 GeV, less than 110 GeV)
Refining Plots with tt̅ Simulation (cont.) Other cuts – Transverse momentum of jets greater than 40 GeV
Refining Plots with tt̅ Simulation (cont.) Other cuts – Missing transverse energy greater than 30 GeV
Refining Plots with tt̅ Simulation (cont.) Other cuts – Cosine of muon angle with beamline between and +0.7
Refining Plots with tt̅ Simulation (cont.) Applying all cuts does get all tt̅ simulation and no background
Application to Data Plots Immediate problem!
Application to Data Plots (cont.) Main cause is stringent requirement on jets – Relax jet constraints to at least two non-b jets and at least one b jet – Keep all other cuts – Note low number of events kept
Conclusions Top mass becomes apparent from decay mode constraints – Other cuts are refinements tt̅ event rarity makes obtaining large numbers of good quality events difficult – Kept about 30 from around 400,000 – Several other data sets that this analysis may be applicable to
Into the Future Mass analysis for other half of tt̅ decay mode – Muon, neutrino, and b jet – MET from neutrino means more challenge Documentation and data archiving Calculating cross-section Changes to Plotter and/or general program structure