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The development in our understanding of symmetry principles is reviewed. Many symmetries, such as charge conjugation, parity and strangeness, are no longer considered as fundamental but as natural consequences of a gauge field theory of strong and electromagnetic interactions. Other symmetries arise naturally from physical models in some limiting situation, such as for low energy or low mass. Random dynamics and attempts to explain all symmetries - even Lorentz invariance and gauge invariance - without appealing to any fundamental invariance of the laws of nature are discussed. A selection of

514.1 --- 514.1 General geometry --- General geometry --- Nucleaire reacties --- Nuclear transmutations --- Partikels (Kernfysica) --- Particles (Nuclear physics) --- Standard model (Nuclear physics) --- Symmetry (Physics) --- Invariance principles (Physics) --- Symmetry (Chemistry) --- Conservation laws (Physics) --- Physics --- Elementary particles (Physics) --- High energy physics --- Nuclear particles --- Nucleons --- Nuclear physics --- Nuclear models --- Nuclear reactions --- Nuclear reactions.

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fysicochemie --- Electronics and optics of solids --- Mathematical physics --- Chemical and physical cristallography --- Symmetry (Physics) --- Energy-band theory of solids --- 512.54 --- 539.21 --- Group theory --- #WSCH:AAS2 --- Invariance principles (Physics) --- Symmetry (Chemistry) --- Conservation laws (Physics) --- Physics --- Groups, Theory of --- Substitutions (Mathematics) --- Algebra --- Band theory of solids --- Conduction band --- Crystallography, Mathematical --- Electrons --- Exciton theory --- Molecules --- Quantum theory --- Solids --- Wave mechanics --- Groups. Group theory --- Properties of molecular systems --- 539.21 Properties of molecular systems --- 512.54 Groups. Group theory --- Chemical and physical crystallography --- Group theory. --- Symmetry (physics)