Physicists use cuts to select events of interest. Cuts preferentially remove the unwanted processes (background) but leave as much as possible of the desired process (signal). It is useful to have a good understanding of the physics processes involved when applying cuts.
We have created two Histogram Analysers, to help visualise the data:
The first Histogram Analyser displays just simulated events.
The second Histogram Analyser displays both real data and simulated events. Both histogram analysers display four physics processes.
The four processes are , , and .
These processes are discussed in the next chapter. Each process is represented by a different colour in Histogram Analyser.
Make cuts using your cursor.
Use the cursor to select a specific range in one of the histograms.
The selected ranges will be coloured, whilst non-selected ranges will be greyed out. When you make cuts on a variable the relative contributions of the four processes will change.
To clear your selection on a specific histogram click on the white background within the histogram area.
To clear all your selections click on "Histogram Analyser" under Get Started in the main top menu.
The histograms explained
Higgs to WW - simulated data Histogram Analyser displays nine histograms. The description of each follows.
Expected Number of Events for 1/fb
This histogram shows the number of events expected to be detected, reconstructed and recorded by ATLAS for 1 inverse femtobarn (1/fb) of data.
One inverse femtobarn corresponds to approximately 100 trillion proton-proton collisions.
The expected number of events reconstructed and recorded by ATLAS is different to the number of events produced.
Some events will not be reconstructed due to the way the detector is constructed, the resolution of the sub-detectors, reconstruction efficiency and other inefficiencies.
The significance of the events quantifies how "significant" the Higgs sample is with respect to the background. It is calculated by ).
The larger the significance value is, the better job you have done extracting the Higgs signal.
The leptonic decay channels are shown here: dielectron (ee), dimuon (mm) and electron-muon (em).
Decays to taus or hadrons are not considered in Histogram Analyser.
Histogram Analyser showing just simulated data, displays three leptonic channels. Histogram Analyser showing simulated and real data, displays just the electron-muon channel, so this histogram is not displayed.
Reconstructed Dilepton Mass [GeV]
This histogram displays the mass reconstructed from the two leptons in the final state.
With no cuts, this peaks at 90 GeV, due the huge boson contribution.
We can remove a large number of boson events by selecting Reconstructed Dilepton Massto be less than 75 GeV, whilst hardly touching our Higgs signal.
The sample significance increases from 0.021 to 0.110 with this cut.
It is thus a useful quantity to use to reduce the huge boson background.
Number of Jets
Number of jets found in the event.
When selecting two or more jets we see that the boson contribution decreases (from 611276 to 25422) and the contribution becomes more important.
Selecting two or more jets, the ratio of ttbar to events increases from 1334/611276 = 0.002 to 1038/25422 = 0.04 and the green ttbar contribution is now noticeable in the histograms.
Top-quark pair production leads to +jets final states.
Are Jets b-tagged?
Jets originating from -quarks are identified and labelled, or tagged, using so-called b-tagging algorithms.
-tagged jets are expected in top quark decays, but not in leptonic or boson decays.
Selecting 'Are Jets b-tagged' as yes, the ratio of ttbar to events increases from 1334/611276 = 0.002 to 1041/7227 = 0.14 and the green ttbar contribution is now noticeable in the histograms.
Missing Transverse Momentum (MET) [GeV]
In the LHC, the initial energy of the colliding partons (quarks or gluons) along the beam axis is not known.
This is due to the energy of each proton being shared and constantly exchanged between its constituents.
However, the initial momentum of particles travelling transverse to the beam axis is zero.
Therefore, any net momentum in the transverse direction indicates missing transverse momentum.
Missing transverse momentum is used to infer the presence of non-detectable particles such as the neutrino.
It is also expected to be a signature of many predicted physics events beyond the Standard Model, for example the lightest supersymmetric particle.
The standard abbreviation for missing transverse momentum is MET, for historical reasons.
Select missing transverse momentum and watch how the ratio of and ttbar to events changes.
Total Lepton Transverse Momentum [GeV]
This is the vectorial sum of the transverse momenta of the observed charged leptons.
For boson events, total lepton transverse momentum peaks at zero since the transverse momenta of both leptons cancel each other.
For the other processes this cancellation is not as pronounced.
Their distributions peak at between 30 and 80 GeV.
Opening Angle Between Leptons [phi]
This is the opening angle, measured in phi (𝜙), between the two leptons.
The azimuthal angle is measured from the -axis, around the beam.
If the leptons are emitted back-to-back, this is displayed on the histogram as 180 degrees.
events show a peak at low values in contrast to all other processes.
Opening Angle Between MET and Leptons [phi]
This is the opening angle, measured in phi (𝜙), between the missing transverse momentum (MET) and the two leptons.
In the event display above, missing transverse energy is displayed by the dotted yellow line. The midline between the two lepton tracks (the direction of the vectorial sum of their transverse momenta) is represented by the dotted red line. The opening angle between the MET and leptons is shown in yellow.
Events with and show a relatively flat distribution in this variable whereas and peak at large values.
This is a useful discriminant to remove background events.