The observed and expected 95% confidence level (CL) limits on the cross-section times branching ratio to diboson final states for the Heavy Vector Triplet (W', Z') scenario, compared to the theoretical predictions for the HVT model-A (red line) and model-B (purple line). (Image: ATLAS Experiment/CERN)

ATLAS has published hundreds of studies of LHC data, with the Higgs boson discovery being perhaps the best known. Amongst the Run 1 searches there was one which stood out: the diboson excess. This was a search for a particle like a W boson but much heavier, decaying into a WZ pair, which then decay into leptons or quarks. The data in the all-quark search showed an excess at 2 TeV, with a local significance of 3.4 sigma (2.5 sigma global significance when the “look-elsewhere” effect is considered). And at the other side of the LHC ring, CMS data seemed to show a small excess at the same place.

This sort of search is rather new. At previous hadronic colliders, the decay of W and Z bosons to quarks has been extremely difficult to observe over the background of quark jets produced directly in the proton collisions. But at the LHC, hadronic boson reconstruction has become a standard tool. Could it be a 2 TeV W' boson? Maybe – but a combination of several W/Z boson decay modes dampened enthusiasm as the other channels showed no excess. Nevertheless, expectations for 2015 were high.

The combined search that has just been published is twice as sensitive to a 2 TeV W' boson as the 2012 result.

The increased LHC beam energy in 2015 meant that heavy objects would be made much more easily. Many possible decay modes of the W and Z were searched for – all but the fully leptonic mode, which is the rarest. The combined search that has just been published is twice as sensitive to a 2 TeV W' boson as the 2012 result.

This combination shows a remarkable understanding of the 2015 data, with delicate analyses demonstrating excellent agreement in control regions. The plot shows the limit set as a function of mass compared with expectation – and at 2 TeV the limit is very close to that expected from background. There is no sign of the 2012 peak.

The analyses have been thoroughly checked to ensure they are robust. So it seems this was just a statistical fluctuation – the known and expected laws of chance. As we consider today a similar situation in the 750 GeV diphoton resonance, we will soon find out if it is just chance or maybe something more…


  1. Search for high-mass diboson resonances with boson-tagged jets in proton-proton collisions at s√ = 8 TeV with the ATLAS detector (arXiv:1506.00962) (J. High Energy Phys. 12 (2015) 55): and
  2. Combination of searches for WW, WZ, and ZZ resonances in pp collisions at s√=8 TeV with the ATLAS detector (arXiv:1512.05099) (Phys. Lett. B 755 (2016) 285-305): and
  3. Searches for heavy diboson resonances in pp collisions at s√=13 TeV with the ATLAS detector (arXiv:1606.04833):
  4. Search for resonances in diphoton events at s√=13 TeV with the ATLAS detector (arXiv: 1606.03833):