LHC di-dijet excesses as signals of fourth-generation tetraquarks

Abstract

We postulate that the excesses of di-dijet events observed at the LHC are attributed to the production of four fourth-generation quarks $b^{\prime }$ with a mass $m_{b^{\prime }}\approx 2$ TeV at few-TeV scales. The di-dijet signals around the four-jet invariant mass $m_{4j}\approx 8$ TeV arise from a resonant $b^{\prime }{b}^{\prime }{\bar{b}}^{\prime }{\bar{b}}^{\prime }$ tetraquark production, where the dijet resonances of masses about 2 TeV correspond to $b^{\prime }{\bar{b}}^{\prime }$ first excited states (color-octet scalars with the principal quantum number $n=2$) in a Yukawa potential created by Higgs boson exchanges. Those around $m_{4j}\approx 3.6$ TeV originate from a non-resonant $b^{\prime }{b}^{\prime }{\bar{b}}^{\prime }{\bar{b}}^{\prime }$ production, where the dijet resonances of masses 0.95 TeV correspond to $b^{\prime }{\bar{b}}^{\prime }$ ground states (color-octet vectors with $n=1$). It is shown that a $b^{\prime }{\bar{b}}^{\prime }$ system with $m_{b^{\prime }}\approx 2$ TeV in the Yukawa potential does generate the aforementioned bound state spectrum. We then illustrate that the observed excesses can be accommodated in our setup by translating the fourth-generation model to the effective theories containing color-octet scalars and vectors available in the literature. The di-dijet events at $m_{4j}=6.6$ TeV and 5.8 TeV with dijet masses about 2 TeV can also be interpreted in the same framework. Simply speaking, our scenario can be viewed as a TeV-scale version of the search for a fully charmed tetraquark via the four-muon channels $X(6900)\to (c\bar{c})(c\bar{c})\to 4\mu$ at a GeV scale.

Comments: 10 pages, 2 figures