Finite Relativity

Today, Feb. 20, 2004, is the 18th birthday of my note "The Relativity Problem in Finite Geometry" shown below.

That note begins with a quotation from Weyl:

"This is the relativity problem: to fix objectively a class of equivalent coordinatizations and to ascertain the group of transformations S mediating between them."
-- Hermann Weyl, The Classical Groups, Princeton University Press, 1946, p. 16

Here is another quotation from Weyl, on the profound branch of mathematics known as Galois theory, which he says

"... is nothing else but the relativity theory for the set Sigma, a set which, by its discrete and finite character, is conceptually so much simpler than the infinite set of points in space or space-time dealt with by ordinary relativity theory."
-- Weyl, Symmetry, Princeton University Press, 1952, p. 138

This second quotation applies equally well to the much less profound, but more accessible, part of mathematics described in Diamond Theory and in my note below.

Related material:

Invariants 

"What modern painters are trying to do,
if they only knew it, is paint invariants."

-- James J. Gibson in Leonardo
(Vol. 11, pp. 227-235.
Pergamon Press Ltd., 1978)

An example of invariant structure:

The three line diagrams above result from the three partitions, into pairs of 2-element sets, of the 4-element set from which the entries of the bottom colored figure are drawn.  Taken as a set, these three line diagrams describe the structure of the bottom colored figure.  After coordinatizing the figure in a suitable manner, we find that the line diagrams are invariant under the group of 16 binary translations acting on the colored figure.

For another sort of invariance of the colored figure, try applying a symmetry of the square to each of the set of four diagonally-divided squares from which the figure's entries are drawn, and observe the induced effect on the figure itself.

A more remarkable invariance -- that of symmetry itself -- is observed if we arbitrarily and repeatedly permute rows and/or columns and/or 2x2 quadrants of the colored figure above. Each resulting figure has some ordinary or color-interchange symmetry. The cause of this symmetry-invariance in the colored patterns is the symmetry-invariance of the line diagrams under a group of 322,560 binary affine transformations.

For more details on the above invariant structures, see Geometry of the 4x4 Square, the Diamond 16 Puzzle, and Diamond Theory.

Also perhaps relevant:

For another perspective, see Block Designs in Art and Mathematics.

Weyl's set Sigma is a finite set of complex numbers.   Some other sets with "discrete and finite character" are those of 4, 8, 16, or 64 points, arranged in squares and cubes.  For illustrations, see Finite Geometry of the Square and Cube.  What Weyl calls "the relativity problem" for these sets involves fixing "objectively" a class of equivalent coordinatizations.  For what Weyl's "objectively" means, see the article "Symmetry and Symmetry  Breaking," by Katherine Brading and Elena Castellani, in the Stanford Encyclopedia of Philosophy:

"The old and natural idea that what is objective should not depend upon the particular perspective under which it is taken into consideration is thus reformulated in the following group-theoretical terms: what is objective is what is invariant with respect to the transformation group of reference frames, or, quoting Hermann Weyl (1952, p. 132), 'objectivity means invariance with respect to the group of automorphisms [of space-time].^'[22]

22. The significance of the notion of invariance and its group-theoretic treatment for the issue of objectivity is explored in Born (1953), for example. For more recent discussions see Kosso (2003) and Earman (2002, Sections 6 and 7).

References:

Born, M., 1953, "Physical Reality," Philosophical Quarterly, 3, 139-149. Reprinted in E. Castellani (ed.), Interpreting Bodies: Classical and Quantum Objects in Modern Physics, Princeton, NJ: Princeton University Press, 1998, pp. 155-167.

Earman, J., 2002, "Laws, Symmetry, and Symmetry Breaking; Invariance, Conservation Principles, and Objectivity,' PSA 2002, Proceedings of the Biennial Meeting of the Philosophy of Science Association 2002, forthcoming [Abstract/Preprint available online]

Kosso, P., 2003, "Symmetry, objectivity, and design," in K. Brading and E. Castellani (eds.), Symmetries in Physics: Philosophical Reflections, Cambridge: Cambridge University Press, pp. 410-421.

Weyl, H., 1952, Symmetry, Princeton, NJ: Princeton University Press.

On relativity theory as "theory of invariants"--

See Archives Henri Poincaré (research unit UMR 7117, at Université Nancy 2, of the CNRS)--

"Minkowski, Mathematicians, and the Mathematical Theory of Relativity," by Scott Walter, in The Expanding Worlds of General Relativity (Einstein Studies, volume 7), H. Goenner, J. Renn, J. Ritter and T. Sauer, editors, Boston/Basel: Birkhäuser, 1999, pp. 45-86--

"Developing his ideas before Göttingen mathematicians in April 1909, Klein pointed out that the new theory based on the Lorentz group (which he preferred to call 'Invariantentheorie') could have come from pure mathematics (1910: 19). He felt that the new theory was anticipated by the ideas on geometry and groups that he had introduced in 1872, otherwise known as the Erlangen program (see Gray 1989: 229)."

References:

Gray, Jeremy J. (1989). Ideas of Space. 2d ed. Oxford: Oxford University Press.

Klein, Felix. (1910). "Über die geometrischen Grundlagen der Lorentzgruppe." Jahresbericht der deutschen Mathematiker-Vereinigung 19: 281-300. [Reprinted: Physikalische Zeitschrift 12 (1911): 17-27].

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Update of Feb. 20, 2008:

For some remarks on the relativity problem in the simpler case of a 2x2x2 cube rather than a 4x4 square, see Knight Moves: Geometry of the Eightfold Cube.

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Page created Feb. 21, 2004