The ATLAS Experiment at @CERN@twitter.com casts wide net in the search for new, high-mass particles! 
Physicists performed an extensive search for these new particles, which are predicted by several #newphysics theories. Learn more in our new briefing 
https://atlas.cern/Updates/Briefing/Search-High-Mass-Particles
ATLASATLAS casts wide net in search for new high-mass particlesSearching for the unknown characteristics of the Universe requires a bit of back-and-forth. Sometimes, experimental physicists drive the effort by discovering something that is not predicted by existing theoretical models. At other times, theorists lead the way by developing models that address gaps in our understanding of Nature. These models often predict the existence of new particles that might be discovered at the LHC, such as those forming dark matter or "graviton" particles predicted in models of the gravitational force. Figure 1: The transverse mass distribution of the electron, muon and neutrinos from VBF events. The data (black dots) and the expected contributions from various background processes (coloured regions) are shown. A NWA particle with a mass of 1 TeV would show up as an excess in the plot above a transverse mass between 400 GeV and 1 TeV (lime green histogram line). (Image: ATLAS Collaboration/CERN) In a new result, the ATLAS Collaboration exploited the full potential of the LHC Run-2 dataset to perform an extensive search for new, high-mass particles that can decay to a pair of W bosons. As many theoretical models predict the existence of such high-mass particles, physicists were able to investigate the validity of several models at once across a large energy range. For their search, physicists focused on two possible production processes for new, high-mass particles: gluon-gluon fusion (ggF) and vector boson fusion (VBF). In the ggF process, two gluons (one from each colliding LHC proton) form the new particle; in the VBF process, each proton radiates a vector boson (either a Z boson or a W boson), which subsequently collide to produce the new particle. In either case, the new particle would quickly decay to a pair of W bosons, which then subsequently decay to an electron, a muon and two neutrinos. Researchers looked at the transverse mass distribution – a mathematical combination of the momentum and energy of the electron, muon and neutrinos – for a signal from the new particle (see Figure 1). The ATLAS Collaboration's new search sets valuable constraints on several theoretical models, pointing future researchers towards new areas for exploration. Figure 2: Upper limits on the ggF production and decay of an excited KK graviton with a 95% confidence level. The black dots show the data. The dotted line is the expectation from the background simulation, and the green and yellow bands are the 1 and 2 standard deviation uncertainties, respectively. The red line is the expected value if a KK graviton exists and the location where the red line crosses the data gives a 95% probability that the minimum possible mass of the KK graviton is 1420 GeV.(Image: ATLAS Collaboration/CERN) However, there are many other types of collisions and decays that also produce an electron, a muon and two neutrinos. These are considered background processes that can obscure possible signals of a new particle. Much of the difficult work in this ATLAS search involved achieving an accurate understanding of the background processes, and optimising selection criteria to separate them from any signals from a new particle. Physicists compared their data to the expected signals of five different theoretical models: a narrow width approximation model (NWA), where the new particle has properties similar to a heavier version of the Standard-Model Higgs boson; a Georgi-Machacek (GM) model, with five predicted Higgs-like particles; a Radion particle, predicted by Randall-Sundrum gravitational models; a heavy vector triplet (HVT) model, consisting of additional Z and W bosons; and an excited Kaluza-Klein (KK) graviton particle, predicted by certain quantum theories of gravity (see Figure 2). As no excess of events was seen above the expected background, ATLAS physicists were able to exclude the existence of all of these new particles below certain mass thresholds, within the bounds of their models. ATLAS’ new result sets valuable constraints on several theoretical models, pointing future researchers towards new areas for exploration. Future searches of the LHC Run 3 dataset may yet yield exciting new insights into the universe. About the event display: Candidate event display of the production of a heavy neutral particle via fusion of two vector bosons, where a jet resulting from a second quark would be outside the detector acceptance and thus not visible. The display shows the resulting signature with one electron (green track), one muon (red line), one jet (within detector acceptance, yellow cone), and a large amount of missing transverse momentum (dashed line). The transverse mass of the system of the electron, muon and missing transverse momentum is 1.4 TeV, which is a lower bound for the mass of the hypothetical heavy particle. (Image: ATLAS Collaboration) Learn more Search for heavy resonances in the decay channel W+W−→eνμν in proton-proton collisions at 13 TeV using 139 fb−1 of data with the ATLAS detector (ATLAS-CONF-2022-066) Higgs 2022 presentation by Pawel Jan Klimek: (ATLAS+CMS) Charged and neutral Higgs-like particles Higgs 2022 presentation by Ke Li: Searches for additional Higgs bosons in ATLAS See also the full lists of ATLAS Conference Notes and ATLAS Physics Papers.
