From ATLAS: “Particle-hunting at the energy frontier”
20th March 2017
Fig. 1: The highest-mass dijet event measured by ATLAS (mass = 8.12TeV). Green lines indicate tracks of charged particles. Green and yellow blocks show the energy of the two back-to-back jets deposited in the calorimeters. (Image: ATLAS Collaboration/CERN)
There are many mysteries the Standard Model of particle physics cannot answer. Why is there an imbalance between matter and anti-matter in our Universe? What is the nature of dark matter or dark energy? And many more. The existence of physics beyond the Standard Model can solve some of these fundamental questions. By studying the head-on collisions of protons at a centre-of-mass energy of 13 TeV provided by the LHC, the ATLAS Collaboration is on the hunt for signs of new physics.
Fig. 2: Dijet resonance search results. (Image: ATLAS Collaboration/CERN)
A newly released ATLAS search studies approximately 30 million collision events that produce two high-energy sprays of particles in the final state. These sprays are known as “jets” or, when seen in pairs as in this case, “dijets” (Figure 1). Jets with extraordinarily high energies – copiously produced due to the strong interactions of quarks and gluons – probe the highest energy scales of all processes at the LHC. These jets can provide a window into new physics phenomena, and allow ATLAS physicists to search for mediators between Standard Model and dark matter particles or other hypothetical objects such as non-elementary quarks, heavy “partners” of known Standard Model particles or miniature quantum black-holes (a phenomenon of strong gravity predicted in models with additional spatial dimensions). They can even be used to search for very heavy particles with masses beyond the LHC collision energies, through models known as contact interactions (similar to the Fermi model for weak interactions).
The dijet search described here consists of two complementary analyses: the resonance analysis and the angular analysis. The resonance analysis looks for a localized excess in the dijet mass spectrum. In the absence of a heavy resonance, the mass distribution is well described by a smooth, monotonically falling function. A statistically significant bump would signify a new particle with mass near the measured bump. The histogram in Figure 2 displays the results of the resonance analysis. The x-axis represents the dijet mass (mjj) and the y-axis (shown with a logarithmic scale) represents the number of observed events. The solid black dots show the data, the red curve represents the fit of a smooth function to the data, and the open green dots show how two non-elementary (“excited”) quark signals might look like. The second panel shows how significant the deviations in the data are as compared to the smooth background fit. The vertical blue lines show the region with the largest significance. A statistical analysis results in a probablility value of 0.63 which means that there is no significant deviation from the Standard Model. The third panel compares the data to the dijet mass prediction; again, no significant deviation from the Standard Model expectation is seen.
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