ATLAS reports first observation of WWW production

26 July 2021 | By

The ATLAS Collaboration announces the first observation of “WWW production”: the simultaneous creation of three massive W bosons in high-energy LHC collisions.

As a carrier particle of the electroweak force, the W boson plays a crucial role in the Standard Model of particle physics. Though discovered nearly four decades ago, the W boson continues to provide physicists with new avenues for exploration. In particular, its study has allowed scientists to test the Standard Model through precise measurements of rare processes.

Today, at the EPS-HEP Conference 2021, the ATLAS Collaboration announced the first observation of a rare process: the simultaneous production of three W bosons. ATLAS researchers analysed the full LHC Run-2 dataset, recorded by the detector between 2015 and 2018, to observe the process with a statistical significance of 8.2 standard deviations – well above the 5 standard-deviation threshold needed to claim observation. This result follows an earlier observation by the CMS Collaboration of inclusive three weak boson production.

Achieving this level of precision was no mean feat. Physicists analysed around 20 billion collision events recorded and pre-filtered by the ATLAS experiment, looking for just a few hundred events expected from the WWW process. These events were buried in almost five times more background events that mimic the signal signature.


The ATLAS Collaboration has observed this process with a statistical significance of 8.2 standard deviations – well above the 5 standard-deviation threshold needed to claim observation.


As one of the heaviest known elementary particles, the W boson is able to decay in several different ways. ATLAS physicists focused their search on the four WWW decay modes with the best discovery potential, due to their reduced number of background events. In three of these modes, two W bosons decay into charged leptons (electrons or muons), carrying the same positive or negative charge, and neutrinos, while the third W boson decays into a pair of light quarks (called the “2l channels”). In the fourth decay mode, all the three W bosons decay into a charged lepton and neutrino (called the “3l channel”).

Physics,ATLAS
The distribution of the BDT variable for data and the Monte Carlo prediction of WWW production in the 3-lepton channel. The expected WWW signal is shown in yellow and the data points are shown in black. (Image: ATLAS Collaboration/CERN)

To pick out the WWW signal from the large number of background events, researchers utilised a machine learning technique called Boosted Decision Trees (BDTs). BDTs can be trained to identify specific signals in the ATLAS detector, spotting small – but key – differences between well-known variables. For this analysis, physicists trained two BDTs: one for the 2l channels using 12 well-modelled variables, and the other for the 3l channel with 11 variables.

The figure shows the BDT distribution for the 3l channel. The improved separation power between signal and background provided by the BDT – along with the massive dataset provided by Run 2 of the LHC – improved the precision of the overall measurement and enabled the first observation of WWW. The observed significance of the measurement is 8.2 standard deviations. The cross section was measured to be 850 ± 100 (statistical) ± 80 (systematic) fb, compared to the Standard Model predicted cross-section of 511 ± 42 fb.

This exciting measurement also allows physicists to look for hints of new interactions that might exist beyond the current energy reach of the LHC. In particular, physicists can use the WWW production process to study the quartic gauge boson coupling, a key parameter of the Standard Model. New particles could alter the quartic gauge boson coupling through quantum effects, modifying the WWW production cross section. The continued study of WWW and other electroweak processes provides an enticing road ahead!


About the event display: Event display of a candidate WWW→ 3 leptons + neutrinos event. The event is identified by its decay to a muon (red line), two electrons (blue lines), and missing transverse energy (white dashed line).


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