1 / 23

Scale invariance

Scale invariance. Object of which a detail when enlarged becomes (approximately) identical to the object itself. Condition of self-similarity leads to properties defined in fractal dimensions. Examples of scale invariance. Snow flakes. Lungs. Trees. Neurons. Symmetry in art.

parkerj
Download Presentation

Scale invariance

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Scale invariance • Object of which a detail when enlarged becomes (approximately) identical to the object itself. Condition of self-similarity leads to properties defined in fractal dimensions. Symmetries in Nuclei, Tokyo, 2008

  2. Examples of scale invariance Snow flakes Lungs Trees Neurons Symmetries in Nuclei, Tokyo, 2008

  3. Symmetry in art • Symmetric patterns are present in the artistry of all peoples. • Symmetry of Ornaments (Speiser, 1927): analysis of group-theoretic structure of plane patterns. Symmetries in Nuclei, Tokyo, 2008

  4. Symmetries of patterns • Four (rigid) trans-formations in a plane: • Reflections • Rotations • Translations • Glide-reflections Symmetries in Nuclei, Tokyo, 2008

  5. One-dimensional patterns Symmetries in Nuclei, Tokyo, 2008

  6. Two-dimensional patterns Symmetries in Nuclei, Tokyo, 2008

  7. Group theory • Group theory is the mathematical theory of symmetry. • Group theory was invented (discovered?) by Evariste Galois in 1831. • Group theory became one of the pillars of mathematics (cfr. Klein’s Erlangen programme). • Group theory has become of central importance in physics, especially in quantum physics. Symmetries in Nuclei, Tokyo, 2008

  8. The birth of group theory • Are all equations solvable algebraically? • Example of quadratic equation: • Babylonians (from 2000 BC) knew how to solve quadratic equations in words but avoided cases with negative or no solutions. • Indian mathematicians (eg. Brahmagupta 598-670) did interpret negative solutions as `depths’. • Full solution was given in 12th century by the Spanish Jewish mathematician Abraham bar Hiyya Ha-nasi. Symmetries in Nuclei, Tokyo, 2008

  9. The birth of group theory • No solution of higher equations until dal Ferro, Tartaglia, Cardano and Ferrari solve the cubic and quartic equations in the 16th century. • Europe’s finest mathematicians (eg. Euler, Lagrange, Gauss, Cauchy) attack the quintic equation but no solution is found. • 1799: proof of non-existence of an algebraic solution of the quintic equation by Ruffini? Symmetries in Nuclei, Tokyo, 2008

  10. The birth of group theory • 1824: Niels Abel shows that general quintic and higher-order equations have no algebraic solution. • 1831: Evariste Galois answers the solvability question: whether a given equation of degree n is algebraically solvable depends on the ‘symmetry profile of its roots’ which can be defined in terms of a subgroup of the group of permutations Sn. Symmetries in Nuclei, Tokyo, 2008

  11. The insolvability of the quintic Symmetries in Nuclei, Tokyo, 2008

  12. The axioms of group theory • A set G of elements (transformations) with an operation  which satisfies: • Closure. If g1 and g2 belong to G, then g1g2 also belongs to G. • Associativity. We always have (g1g2)g3=g1(g2g3). • Existence of identity element. An element 1 exists such that g1=1g=g for all elements g of G. • Existence of inverse element. For each element g of G, an inverse element g-1 exists such that gg-1=g-1g=1. • This simple set of axioms leads to an amazingly rich mathematical structure. Symmetries in Nuclei, Tokyo, 2008

  13. Example: equilateral triangle • Symmetry trans-formations are • - Identity • - Rotation over 2/3 and 4/3 around ez • Reflection with respect to planes (u1,ez), (u2,ez), (u3,ez) • Symmetry group: C3h. Symmetries in Nuclei, Tokyo, 2008

  14. Groups and algebras • 1873: Sophus Lie introduces the notion of the algebra of a continuous group with the aim of devising a theory of the solvability of differential equations. • 1887: Wilhelm Killing classifies all Lie algebras. • 1894: Elie Cartan re-derives Killing’s classification and notices two exceptional Lie algebras to be equivalent. Symmetries in Nuclei, Tokyo, 2008

  15. Lie groups • A Lie group contains an infinite number of elements characterized by a set of continuous variables. • Additional conditions: • Connection to the identity element. • Analytic multiplication function. • Example: rotations in 2 dimensions, SO(2). Symmetries in Nuclei, Tokyo, 2008

  16. Lie algebras • Idea: to obtain properties of the infinite number of elements g of a Lie group in terms of those of a finite number of elements gi(called generators) of a Lie algebra. Symmetries in Nuclei, Tokyo, 2008

  17. Lie algebras • All properties of a Lie algebra follow from the commutation relations between its generators: • Generators satisfy the Jacobi identity: • Definition of the metric tensor or Killing form: Symmetries in Nuclei, Tokyo, 2008

  18. Classification of Lie groups • Symmetry groups (of projective spaces) over R, C and H (quaternions) preserving a specified metric: • The five exceptional groups G2, F4, E6, E7 and E8 are similar constructs over the normed division algebra of the octonions, O. Symmetries in Nuclei, Tokyo, 2008

  19. Rotations in 2 dimensions, SO(2) • Matrix representation of finite elements: • Infinitesimal element and generator: • Exponentiation leads back to finite elements: Symmetries in Nuclei, Tokyo, 2008

  20. Rotations in 3 dimensions, SO(3) • Matrix representation of finite elements: • Infinitesimal elements and associated generators: Symmetries in Nuclei, Tokyo, 2008

  21. Rotations in 3 dimensions, SO(3) • Structure constants from matrix multiplication: • Exponentiation leads back to finite elements: • Relation with angular momentum operators: Symmetries in Nuclei, Tokyo, 2008

  22. Casimir operators • Definition: The Casimir operators Cn[G] of a Lie algebra G commute with all generators of G. • The quadratic Casimir operator (n=2): • The number of independent Casimir operators (rank) equals the number of quantum numbers needed to characterize any (irreducible) representation of G. Symmetries in Nuclei, Tokyo, 2008

  23. Symmetry rules • Symmetry is a universal concept relevant in mathematics, physics, chemistry, biology, art… • Since its introduction by Galois in 1831, group theory has become central to the field of mathematics. • Group theory remains an active field of research, (eg. the recent classification of all groups leading to the Monster.) • Symmetry has acquired a central role in all domains of physics. Symmetries in Nuclei, Tokyo, 2008

More Related