Abstract

Symmetries in the Physical Laws of Nature lead to observable effects. Beyond the regularities and conserved magnitudes, the last few decades in particle physics have seen the identification of symmetries, and their well-defined breaking, as the guiding principle for the elementary constituents of matter and their interactions. Flavour SU(3) symmetry of hadrons led to the Quark Model and the antisymmetric requirement under exchange of identical fermions led to the colour degree of freedom. Colour became the generating charge for flavour-independent strong interactions of quarks and gluons in the exact colour SU(3) local gauge symmetry. Parity Violation in weak interactions led us to consider the chiral fields of fermions as the objects with definite transformation properties under the weak isospin SU(2) gauge group of the Unifying Electro-Weak SU(2) × U(1) symmetry, which predicted novel weak neutral current interactions. CP-Violation led to three families of quarks opening the field of Flavour Physics. Time-reversal violation has recently been observed with entangled neutral mesons, compatible with CPT-invariance. The cancellation of gauge anomalies, which would invalidate the gauge symmetry of the quantum field theory, led to Quark–Lepton Symmetry. Neutrinos were postulated in order to save the conservation laws of energy and angular momentum in nuclear beta decay. After the ups and downs of their mass, neutrino oscillations were discovered in 1998, opening a new era about their origin of mass, mixing, discrete symmetries and the possibility of global lepton-number violation through Majorana mass terms and Leptogenesis as the source of the matter–antimatter asymmetry in the universe. The experimental discovery of quarks and leptons and the mediators of their interactions, with physical observables in spectacular agreement with this Standard Theory, is the triumph of Symmetries. The gauge symmetry is exact only when the particles are massless. One needs a subtle breaking of the symmetry, providing the origin of mass without affecting the excellent description of the interactions. This is the Brout–Englert–Higgs Mechanism, which produces the Higgs Boson as a remnant, discovered at CERN in 2012. Open present problems are addressed with by searching the New Physics Beyond-the-Standard-Model.

Highlights

  • Symmetries in the Physical Laws of Nature lead to observable effects

  • Knowing that neutrinos are massive, the most fundamental problem is the determination of the nature of neutrinos with definite mass: are they either four-component Dirac particles with a conserved global lepton number L, distinguishing neutrinos from antineutrinos; or two-component truly neutral self-conjugate Majorana particles [98]? For Dirac neutrinos, like quarks and charged leptons, their masses can be generated in the Standard Model of particle physics by spontaneous breaking of the gauge symmetry with the doublet Higgs scalar, if there are additional right-handed sterile neutrinos

  • The particle content was induced by Discrete Symmetry Breaking for fermions, opening the field of Flavour Physics for Quarks and Leptons

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Summary

Symmetry as Guiding Principle for Particles and Interactions

We observe symmetry of objects, like characteristic features of geometrical forms, material objects or biological bodies. Symmetry and Symmetry very important concepts in the field ofhowever elementary particle to objects, but to the Fundamental. Well examples For are momentum for translations, angular momentum for leads to a Covariant This is valid for rotations or charge for gauge symmetry. Gauge group or non-Abelian gauge groups withThis the is interaction leads to a Covariant with a Mediator valid for field transforming as the adjoint representation. In Sectionas2,the weadjoint develop the ideas leading from hadrons to quarks and the symmetries of strong transforming representation. Symmetries, with the observation and implications of the independent breaking plus the third family of bottom and top quarks, including Quark–Lepton Symmetry.

Quarks and Strong of Interactions
Octet and Decuplet
Are Quarks Real?
The Colour Charge
Asymptotic Freedom
Chirality and Electroweak Interaction
GIM Mechanism
The Third Family
Gauge Anomalies
CP Violation
Time Reversal Violation
Experimental in the the entangled entangled B
Neutrinos
The Energy Crisis
14 N should protons and
Lepton Flavours
Neutrino Mass and Mixing
Genuine CP Violation
Global Lepton Number
The Brout–Englert–Higgs Mechanism
The Higgs Boson gauge and Yukawa Couplings
The Higgs Potential
Conclusions and Outlook
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