
Wittgenstein, Minkowski, Riemann, Maxwell, Russell, Whitehead, Kline, Feigl, Brentano, Poincaré, Gödel  

Thus the colors with their various qualities and intensities fulfill the axioms of vector geometry if addition is interpreted as mixing; consequently, projective geometry applies to the color qualities. ~Weyl 

Wittgenstein Minkowski Riemann Weyl Maxwell Russell Whitehead Kline Brentano Feigl Poincaré
Fourier Feynman Nagel Newman 
A speck in the visual field, though it need not be red, must have some color; it is, so to speak, surrounded by color space. Notes must have some pitch, objects of the sense of touch some degree of hardness, and so on. Wittgenstein In the language of
physics, theories where forces are explained in terms of curvature are
called `gauge theories.' Mathematically, the key concept in a gauge
theory is that of a `connection' on a `bundle'. The idea here is to
start with a manifold M describing spacetime. For each point x of
spacetime, a bundle gives a set E_{x} of allowed internal
states for a particle at this point.
Baez
So
few and far between are the occasions for forming notions whose
specializations make up a continuous manifold, that the only simple
notions whose special izations form a multiply extended manifold are
the positions of perceived objects and colors.
§ Definite
portions of a manifold, distinguished by a mark or a boundary, are
called Quanta [...]
Riemann
When
a beam of light falls on the human eye, certain sensations are
produced, from which the possessor of that organ judges of the color
and luminance of the light. Now, though everyone experiences these
sensations and though they are the foundation of all the phenomena of
sight, yet, on account of their absolute simplicity, they are incapable
of analysis, and can never become in themselves objects of thought. If
we attempt to discover them, we must do so by artificial means and our
reasonings on them must be guided by some theory.
Maxwell Mathematics
has introduced the name
isomorphic representation for the relation which according to Helmholtz
exists between objects and their signs. I should like to carry out the
precise explanation of this notion between the points of the projective
plane and the color qualities [...]
the
projective plane and the color
continuum are isomorphic with one another. Every theorem which is
correct in the one system Σ_{1}
is
transferred unchanged to the other Σ_{2}.
A science can never determine its subject matter except up to an
isomorphic representation. The idea of isomorphism indicates the
selfunderstood, insurmountable barrier of knowledge. It follows that
toward the "nature" of its objects science maintains complete
indifference. This for example what distinguishes the colors from the
points of the projective plane one can only know in immediate alive
intuition [...]
Weyl
[It]
became possible to affirm that projective geometry is indeed logically
prior to Euclidean geometry and that the latter can be built up as a
special case. Both Klein and Arthur Cayley showed that the basic
nonEuclidean geometries developed by Lobachevsky and Bolyai and the
elliptic nonEuclidean geometry created by Riemann can also be derived
as special cases of projective geometry. No wonder that Cayley
exclaimed, "Projective geometry is all geometry."
The
principle
of duality
in
projective geometry states that we can interchange point and line in a
theorem about figures lying in one plane and obtain a meaningful
statement. Moreover, the new or dual statement will itself be a
theoremthat is, it can be proven. On the basis of what has been
presented here we cannot see why this must always be the case for the
dual statement. However, it is possible to show by one proof that every
rephrasing of a theorem of projective geometry in accordance with the
principle of duality must be a theorem. This principle is a remarkable
characteristic of projective geometry. It reveals the symmetry in the
roles that point and line play in the structure of that geometry.
Kline "[The] projective plane and the color continuum are isomorphic with one another." (Weyl)
We begin with a piece of late19thcentury physics. The vacuum Maxwell equations for the electric and magnetic fields E and B, have a symmetry under
Witten
Carroll
All
other psychological phenomena are derived from the combinations of
these ultimate psychological elements, as the totality of words may
be derived from the totality of letters. Completion of this task would
provide the basis for a Characteristica
universalis
of the sort that had been conceived by Leibniz, and before him, by
Descartes.
Brentano
How
did
Gödel prove his conclusions?
Up to a point, the structure of his demonstration is modeled, as he
himself noted, on the reasoning involved in one of the logical
antinomies known as the "Richard Paradox," first propounded by the
French mathematician, Jules Richard, in 1905 [...] The reasoning in the
Richard Paradox is evidently fallacious. Its construction nevertheless
suggests that it might be possible to "map" (or "mirror")
metamathematical statements about a sufficiently comprehensive formal
system into the system itself. If this were possible, then
metamathematical statements about a system would be represented by
statements within the system. Thereby one could achieve the desirable
end of getting the formal system to speak about itself—a most valuable
form of selfconsciousness.
The
idea
of such mapping is a
familiar one in mathematics. It is employed in coordinate geometry,
which translates geometric statements into algebraic ones, so that
geometric relations are mapped onto algebraic ones. The idea is
manifestly used in the construction of ordinary maps, since the
construction consists in projecting configurations on the surface of a
sphere onto a plane [...]
The
basic
fact which underlies all
these mapping procedures is that an abstract structure of relations
embodied in one domain of objects is exhibited to hold between
"objects" in some other domain.
In
consequence, deductive relations
between statements about the first domain can be established by
exploring (often more conveniently and easily) the deductive relations
between statements about their counterparts. For example, complicated
geometrical relations between surfaces in space are usually more
readily studied by way of the algebraic formulas for such surfaces.
Newman & Nagel A group in mathematics is an
object that measures symmetry in the same way that a number measures
quantity. As the recent paper
explains, groups can be used to cast light on neoRiemannian theory,
which is a topic in music theory that gives some insight into
progressions of major and minor triad chords.
NeoRiemannian theory is not named after the famous 19thcentury German mathematician Bernhard Riemann, but rather after the German music theorist Hugo Riemann, who lived somewhat later. The three basic operations in the theory, known as P, R and L, transform triad chords into other triad chords as follows. The P transformation exchanges a major triad with the parallel minor triad: for example, it exchanges a C major triad (CEG) with a C minor triad (CE flatG). The R transformation exchanges a major triad with the relative minor triad: for example, it exchanges a C major triad (CEG) with an A minor triad (ACE). The L transformation exchanges a triad for its leadingtone exchange: for example, it exchanges a C major triad (CEG) with an E minor triad (EGB). The animation shows the notes of the scale on a torus. R Green
It turns out that these automorphic sheaves "live" on a certain space attached to a Riemann surface X and the group G, called the moduli space of Gbundles on X. Frenkel 
So
where
a vector is a magnitude and a particular direction from some point, a
tensor gives a magnitude for every direction from that point. A tensor
field is something that assigns a tensor to every point in space.
Riemann calls a system in which one individual can be determined by n measurments an n fold extended aggregate, or an aggregate of n dimensions. Thus the space in which we live is a threefold, a surface is a twofold, and a line is a simple extended aggregate of points. Time also is an aggregate of one dimension. The system of colors is an aggrgate of three dimensions, inasmuch as each color, according to the investigations of Thomas Young and Clerk Maxwell, may be represented as a mixture of three primary colors in definite quantities. Helmholtz
It is easy to imagine a global color symmetry. The quark colors, like the isotopicspin states of hadrons, might be indicated by the orientation of an arrow in some imaginary internal space. 't Hooft If antipodal points have 180 degrees of phase difference, adding them gives 'darkness,' or 'no light,' or 'zero.' We then have a natural inverse operation — all we need to give colors a group structure, the other requirements being obviously met. A geometricalphysical theory as such is incapable of being directly pictured, being merely a system of concepts. But these concepts serve the purpose of bringing a multiplicity of real or imaginary sensory experiences into connection in the mind. To "visualize" a theory therefore means to bring to mind that abundance of sensible experiences for which the theory supplies the schematic arrangement. Einstein We will try to visualize the state of things by the graphic method. Let x, y, z be rectangular coordinates for space, and let t denote time. The objects of our perception invariably include places and times in combination. Nobody has ever noticed a place except at a time, or a time except at a place. [...] The multiplicity of all thinkable x, y, z, t systems of values we will christen the world. Minkowski The characteristic of an ndimensional manifold is that each of the elements composing it (in our examples, single points, conditions of a gas, colors, tones) may be specified by the giving of n quantities, the "coordinates," which are continuous functions within the manifold. §
We said at an earlier place, that every difference in experience must be founded on a difference of the objective conditions; we can now add: in such a difference of the objective conditions as is invariant with regard to coordinate transformations, a difference that cannot be made to vanish by a mere change of the coordinate system used. Weyl
CalabiYau space Weyl § The feeling of an
unbridgeable gulf between consciousness and brainprocess: how does it
come about that this does not come into the considerations of our
ordinary life? This idea of a difference in kind is accompanied by
slight giddiness — which occurs when we are performing a piece of
logical sleightofhand. [...] When does this feeling occur in the
present case? It is when I, for example, turn my attention in a
particular way on to my own consciousness, and, astonished, say to
myself: THIS is supposed to be produced by a process in the brain! Wittgenstein
Thus "this is red," "this
is earlier than that," are
Some of the early work was motivated by the hope that the fifth dimension could provide the hidden variables that would eliminate indeterminacy from quantum mechanics. Despite the many generalizations amd changes in emphasis that have occurred, I will refer generically to theories in which gauge fields are unified with gravitation by means of extra, compact dimensions as KaluzaKlein theories. Witten I can here only briefly indicate the lines along which I think the 'world knot' — to use Schopenhauer's striking designation for the mindbody puzzles may be disentangled. The indispensable step consists in a critical reflection upon the meanings of the terms 'mental' and 'physical', and along with this a thorough clarification of such traditional philosophical terms as 'private' and 'public', 'subjective' and 'objective', 'psychological space(s)' and 'physical space', 'intentionality', 'purposiveness', etc. The solution that appears most plausible to me, and that is consistent with a thoroughgoing naturalism, is an identity theory of the mental and the physical, as follows: Certain neuro physiological terms denote (refer to) the very same events that are also denoted (referred to) by certain phenomenal terms. [...] I take these referents to be the immediately experienced qualities, or their configurations in the various phenomenal fields. Feigl
Has this a meaning, and if so what? Does it mean that we represent to ourselves external objects in geometrical space? Our representations are only the reproduction of our sensations; they can therefore be ranged only in the same frame as these, that is to say, in perceptual space. It is as impossible for us to represent to ourselves external bodies in geometric space, as it is for a painter to paint on a plane canvass objects with their three dimensions. Perceptual space is only an image of geometric space, an image altered in shape by a sort of perspective [...] Poincaré
Fortunately the problem is easier for the mathematician than for the analytical chemist. There is a very simple technique for analyzing any curve, no matter how complicated it may be, into its constituent simple harmonic curves. It is based on a mathematical theorem known as Fourier's theorem [...] The theorem tells us that every curve, no matter what its nature may be, or in what way it was originally obtained, can be exactly reproduced by superposing a sufficient number of simple harmonic curves — in brief, every curve can be built up by piling up waves. Sir
James Jeans
Any physical system
is completely described
The
Langlands Program, launched by Robert Langlands in the late 60's, ties
together seemingly unrelated objects in number theory, algebraic
geometry, and the theory of automorphic functions. The Langlands
conjecture predicts that there is a correspondence between
ndimensional representations of the Galois group of a number field and
automorphic representations of the group GL(n) over the ring of adeles
of this field. This conjecture has an analogue when the number
field is replaced by the field of functions on a smooth projective
curve defined over a finite field. In this setting, this
conjecture has a geometric version, called the geometric Langlands correspondence.by a normalized vector (the state vector or wave function) in Hilbert space. ~Byron & Fuller 
gauge tensor
spacetime group HVs projective 

