Discussion Overview
The discussion centers around the detection of the heaviest particle at the Large Hadron Collider (LHC) and the upper limits for the mass of new particles that could potentially be detected. Participants explore the implications of collision energy, parton interactions, and exclusion limits for various particle models, including the Lightest Kaluza-Klein Particle (LKP) and supersymmetry.
Discussion Character
- Technical explanation
- Debate/contested
- Mathematical reasoning
Main Points Raised
- Some participants assert that the heaviest known particle detected is the top quark, with a mass of approximately 172 GeV, followed by the Higgs boson and W/Z bosons.
- It is noted that the LHC operates at a collision energy of 13 TeV, but the actual energy available for producing new particles is limited by the momentum fractions of the colliding partons.
- Participants discuss that producing a new particle requires at least double its mass due to conservation laws, complicating the detection of heavier particles.
- Exclusion limits for various models, including supersymmetry and Kaluza-Klein particles, are mentioned, with some limits being in the low hundreds of GeV range and others exceeding 1 TeV.
- One participant references the need for indirect searches to set limits above the collision energy threshold, particularly in the context of new physics models.
- Links to external resources for exclusion limits and relevant plots from CMS and ATLAS are provided for further exploration of the topic.
Areas of Agreement / Disagreement
Participants generally agree that the top quark is the heaviest particle detected so far, but there are varying views on the implications of collision energy and the limits for detecting new particles. The discussion remains unresolved regarding the specific exclusion limits for Kaluza-Klein particles and the interpretation of the referenced plots.
Contextual Notes
There are limitations regarding the assumptions made about parton momentum fractions and the indirect nature of some exclusion limits. The discussion also highlights the complexity of distinguishing new particle production from background processes.