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  1. en.wikipedia.org › wiki › IsospinIsospin - Wikipedia

    Flavour inparticle physics. In nuclear physics and particle physics, isospin ( I) is a quantum number related to the up- and down quark content of the particle. Isospin is also known as isobaric spin or isotopic spin . Isospin symmetry is a subset of the flavour symmetry seen more broadly in the interactions of baryons and mesons .

  2. Scientists. v. t. e. Particle physics or high-energy physics is the study of fundamental particles and forces that constitute matter and radiation. The field also studies combinations of elementary particles up to the scale of protons and neutrons, while the study of combination of protons and neutrons is called nuclear physics .

  3. The development of the Standard Model was driven by theoretical and experimental particle physicists alike. The Standard Model is a paradigm of a quantum field theory for theorists, exhibiting a wide range of phenomena, including spontaneous symmetry breaking, anomalies, and non-perturbative behavior.

  4. If the MSSM squark masses are flavor-violating, such a process can occur. In particle physics, flavor-changing neutral currents or flavour-changing neutral currents ( FCNCs) are hypothetical interactions that change the flavor of a fermion without altering its electric charge .

  5. Talk:Flavour (particle physics) Talk. : Flavour (particle physics) Flavour (particle physics) has been listed as a level-5 vital article in Science, Physics. If you can improve it, please do. This article has been rated as Start-class on Wikipedia's content assessment scale. This article is written in British English with Oxford spelling ...

  6. This is an audio version of the Wikipedia Article:https://en.wikipedia.org/wiki/Flavour_(particle_physics)00:00:30 1 Quantum numbers00:02:24 1.1 Conservation...

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  7. In particle physics, the GIM mechanism (or Glashow–Iliopoulos–Maiani mechanism) is the mechanism through which flavour-changing neutral currents (FCNCs) are suppressed in loop diagrams. It also explains why weak interactions that change strangeness by 2 (Δ S = 2 transitions) are suppressed, while those that change strangeness by 1 (Δ S ...