Abstract

Recent data collected by ATLAS and CMS at 13 TeV collision energy of the LHC indicate the existence of a new resonant state $\phi$ with a mass of 750 GeV decaying into two photons $\gamma\gamma$. The properties of $\phi$ should be studied further at the LHC and also future colliders. Since only $\phi \to \gamma\gamma$ decay channel has been measured, one of the best ways to extract more information about $\phi$ is to use a $\gamma\gamma$ collider to produce $\phi$ at the resonant energy. In this work we show how a $\gamma\gamma$ collider helps to verify the existence of $\phi$ and to provide some of the most important information about the properties of $\phi$, such as branching fractions of $\phi\to V_1V_2$. Here $V_i$ can be $\gamma$, $Z$, or $W^\pm$. We also show that by studying angular distributions of the final $\gamma$'s in $\gamma\gamma \to \phi \to \gamma\gamma$, one can obtain crucial information about whether this state is a spin-0 or a spin-2 state.

Highlights

  • Recent data collected by ATLAS and CMS at 13 TeV collision energy of the LHC indicate the existence of a new resonant state φ with a mass of 750 GeV decaying into two photons γγ

  • Recent data collected by ATLAS and CMS at s = 13 TeV collision energy of the LHC indicate the existence of a new resonant state φ with a mass of 750 GeV decaying into two photons [1]

  • The production cross section σ(pp → φ → γγ) is about 6 fb with the ATLAS data hinting that φ has a broad width about 45 GeV with a local significance of 3.9σ, while CMS data favor a narrow width of order 100 MeV with a local significance of 2.6σ [1]

Read more

Summary

Iy fb

TeV, the differences for spin-0 and spin-2 laboratory frame angular distribution are substantial. This can be used to distinguish whether φ is a spin-0 or a spin-2 state. For spin-0 case, the distribution is almost flat despite of the boost effect shown in eq(14) in the laboratory frame. This is because that at 1 TeV, the particle produced has a small kinetic energy and it is almost at rest. With the total integrated luminosity to be 1000 fb−1, with information in Figure 2 one would obtain an event number N ∼ 290 for unpolarized case, √.

The error in
Summary
Ni N Ni N
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.