



Elements
II









The reciprocal relationship of epistemology and
science is
of a noteworthy kind. They are
dependent upon each other.
Einstein




A = A
The first fullfledged exposition of a mathematical theory of vision is found in the Optica of Euclid (fl. 300 B.C.). Indeed, Euclid's approach to vision was so strictly mathematical as to exclude all but the most incidental references to those aspects of the visual process not reducible to geometrythe ontology of visual radiation and the physiology and psychology of vision. Lejeune comments that Euclid's Optica systematically ignores every physical and psychological aspect of the problem of vision. It restricts itself to that which can be expressed geometrically. [...] Its model is the treatise on pure geometry, and its method that of the Elements: a few postulates all fully necessary, from which follow deductively and with full mathematical rigor a series of theorems of a traditional form. Lindberg
Thus "this is red," "this is earlier than that," are atomic propositions. Russell & Whitehead
If you ask a physicist what is his idea of yellow light, he will tell you that it is transversal electromagnetic waves of wavelength in the neighborhood of 590 millimicrons. If you ask him: But where does yellow come in? he will say: In my picture not at all, but these kinds of vibrations, when they hit the retina of a healthy eye, give the person whose eye it is the sensation of yellow. Schrödinger ...every element of the physical reality must have a counterpart in the physical theory. EPR
A color is a physical object a soon as we consider its dependence, for instance, upon its luminous source, upon temperatures, and so forth. Mach
The
ultimate of ultimate problems, of course, in the study of the relations
of thought and brain, is to understand why and how such disparate
things are connected at all … We must find the minimal mental
fact whose being reposes directly on a brainfact; and we must
similarly find the minimal brain event which will have a mental
counterpart at all.
William James
The
senseobject is the simplest permanence which we trace as
selfidentical in external events. It is some definite sensedatum,
such as the color red of a definite shade. We see redness here and the
same redness there, redness then and the same redness now. In other
words, we perceive redness in the same relation to various definite
events, and it is the same redness which we perceive. Tastes, colors,
sounds, and every variety of sensation are objects of this sort.
Whitehead
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 "co ordinates," which are continuous functions within the manifold. Weyl
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 neurophysiological 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
This is the characteristic mathematical property of a classical field: it is an undefined something which exists throughout a volume of space and which is described by sets of numbers, each set denoting the field strength and direction at a single point in the space. § There is nothing else except these fields: the whole of the material universe is built of them. Dyson
I would
like to again impress you with the vast range of phenomena that the
theory of quantum electrodynamics describes: It's easier to say it
backwards: the theory describes all the phenomena of the physical world
except the gravitational effect [...] and radioactive phenomena, which
involve nuclei shifting in their energy levels. So if we leave out
gravity and radioactivity (more properly, nuclear physics) what have we
got left? Gasoline burning in automobiles, foam and bubbles, the
hardness of salt or copper, the stiffness of steel. In fact, biologists
are trying to interpret as much as they can about life in terms of
chemistry, and as I already explained, the theory behind chemistry is
quantum electrodynamics.
Feynman
[When]
a state is formed by the superposition of two other states, it will
have properties that are in some vague way intermediate between those
of the original states and that approach more or less closely to those
of either of them according to the greater or less 'weight' attached to
this state in the superposition process. The new state is completely
defined by the two original states when their relative weights in the
superposition process are known, together with a certain phase
difference, the exact meaning of weights and phases being provided in
the general case by the mathematical theory.
Dirac Increasingly,
many of us have come to think that the missing element that has to be
added to quantum mechanics is a principle, or several principles, of
symmetry. A symmetry is a statement that there are various ways that
you can change the way you look at nature, which actually change the
direction the state vector is pointing, but which do not change the
rules that govern how the state vector rotates with time. The set of
all these
changes in point of view is called the symmetry group of nature. It is
increasingly clear that the symmetry group of nature is the deepest
thing that we understand about nature today.
Weinberg
Furthermore, and now this is the point, this is the punch line, the symmetries determine the action. This action, this form of the dynamics, is the only one consistent with these symmetries [...] This, I think, is the first time that this has happened in a dynamical theory: that the symmetries of the theory have completely determined the structure of the dynamics, i.e., have completely determined the quantity that produces the rate of change of the state vector with time. Weinberg
To monochromatic light corresponds in the acoustic domain the simple tone. Out of different kinds of monochromatic light composite light may be mixed, just as tones combine to a composite sound. This takes place by superposing simple oscillations of different frequency with definite intensities. Weyl
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 —
is transferred unchanged to the other. A science
can never determine its subject matter except up to an isomorphic
representation. The idea of isomorphism indicates the self understood,
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
The science of
colors becomes a
speculation as truly
mathematical as any other part of physics. ~Newton
There
is in
the absolute differential calculus a kind of law of reciprocity or
duality in accordance with which we can deduce from every theorem or
formula a reciprocal theorem or formula by interchanging the words
covariant
and contravariant,
and lowering or raising the indices.
LeviCivita
From the above brief
review, we
find there are three versions of geometrization of non gravitational
gauge interactions:
1. Fibrebundle version, in which the gauge interactions are correlated with the geometrical structures of internal space. [...] the essence of the internal space is still a vexing problem: Is it a physical reality as real as spacetime, or just a mathematical structure? 2. KaluzaKlein version, in which extra space dimensions which compactify in lowenergy experiments are introduced and the gauge symmetries by which the forms of gauge interactions are fixed are just the manifestation of the geometrical symmetries of the compactified space. [...] The assumption of the reality of the compactified space is substantial and is in principle testable [...] 3. Superstring version, in which the introduction of extra compactified space dimensions is due to different considerations from just reproducing the gauge symmetry. Cao
While
a proper
understanding of Mtheory still eludes us, much is now known about it.
In particular the various geometric results that
have emerged from string theory become related in interesting but
mysterious ‘dualities’ whose real meaning has yet to be discovered.
Atiyah
The
reciprocal relationship of epistemology and science is of noteworthy
kind. They are dependent upon each other. Epistemology without contact
with science becomes an empty scheme. Science without epistemology is –
insofar as it is thinkable at all – primitive and muddled. However, no
sooner has the epistemologist, who is seeking a clear system, fought
his way through to such a system, than he is inclined to interpret the
thoughtcontent of science in the sense of his system and to reject
whatever does not fit into his system. The scientist, however, cannot
afford to carry his striving for epistemological systematic that far.
He accepts gratefully the epistemological conceptual analysis; but the
external conditions, which are set for him by the facts of experience,
do not permit him to let himself be too much restricted in the
construction of his conceptual world by the adherence to an
epistemological system. He therefore must appear to the systematic
epistemologist as a type of unscrupulous opportunist: he appears as
realist insofar as he seeks to describe a world independent of the acts
of perception; as idealist insofar as he looks upon the concepts and
theories as the free inventions of the human spirit (not logically
derivable from what is empirically given); as positivist insofar as he
considers his concepts and theories justified only to the extent to
which they furnish a logical representation of relations among sensory
experiences. He may even appear as Platonist or Pythagorean insofar as
he considers the viewpoint of logical simplicity as an indispensable
and effective tool of his research.
Einstein


We cannot confuse what to us appears unnatural with the absolutely impossible. ~Gauss 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
A = B
It seems useful to me to develop a little more precisely the "geometry" valid in the twodimensional manifold of perceived colors. For one can do mathematics also in the domain of these colors. The fundamental operation which can be performed upon them is mixing: one lets colored lights combine with one another in space... Weyl
So
few and far between are the
occasions for
forming notions whose specialisations make up a continuous manifold,
that the only simple notions whose
specialisations form a multiply extended manifold are the positions of
perceived objects and colors.
Riemann This leaf (given to me in the
present act of perception) has this
definite green color (given to me in this very perception). ~Weyl
A speck in the visual field, though it need not be red must have some color; it is, so to speak, surrounded by colorspace. Notes must have some pitch, objects of the sense of touch some degree of hardness, and so on. Wittgenstein
It is often said that we "project" into geometric space the objects of our external perception; that we "localize" them. 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
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.
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 The two main approaches
for the description of sound fields are methods derived from solutions
of the wave equation and geometric methods based on analogies to ray
optics. Their mathematical representations are reviewed and it is shown
that representations by projective geometry and descriptions by Fourier
acoustics lead to similar parametric representations of sound fields.
Annibale et al.
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 theorem — that 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
A projection matrix P is an n x n square matrix that gives a vector space projection from R^{n} to a subspace W. The columns of P are the projections of the standard basis vectors, and W is the image of P. A square matrix is a projection matrix iff P^{2} = P. Wolfram MathWorld
Our
basic ontology is that all
systems, macroscopic
structures included, are quantum fields [...]
Saunders
't Hooft
Further,
these laws are very interesting mathematically. For those who are
interested in the mathematics of the thing, it turns out as follows.
Suppose that we take our three colors, which were red, green, and blue,
but label them A, B, and C, and call them our primary colors. Then any
color could be made by certain amounts of these three: say an amount a
of color A, an amount b of color B, and an amount c of color C makes X:
X = aA + bB + cC. Now suppose another color Y is made from the same three colors: Y = a'A + b'B + c'C. Then it turns out that the mixture of the two lights (it is one of the consequences of the laws that we have already mentioned) is obtained by taking the sum of the components of X and Y: Z = X + Y = (a + a')A + (b + b')B + (c + c')C. It
is just like the mathematics of the addition of vectors, where (a, b, c
) are the components of one vector, and (a', b', c' ) are those of
another vector, and the new light Z is then the "sum" of the vectors.
This subject has always appealed to physicists and mathematicians. In
fact, Schrödinger wrote a wonderful paper on color vision in which he
developed this theory of vector analysis as applied to the mixing of
colors. Feynman
How
do convex sets arise? An instructive example occurs in color theory,
and more particularly in the psychophysical theory of color. (This
means that we will leave out the interesting questions about how our
brain actually processes the visual information until it becomes a
percept.) In a way tradition suggests that color theory should be
studied before quantum mechanics, because this is what Schrodinger was
doing before inventing his wave equation. The object of our attention
is color space, whose points are the colors. Naturally one might worry
that the space of colors may differ from person to person but in fact
it does not. The perception of color is remarkably universal for human
beings, color blind persons not included. What has been done
experimentally is to shine mixtures of light of different colors on
white screens; say that three reference colors consisting of red, green
and blue light are chosen. Then what one finds is that after adjusting
the mixture of these colors, the observer will be unable to distinguish
the resulting mixture from a given color C.
~Bengtsson and Zyczkowski
What we learn from our whole discussion and what indeed has become a guiding principle in modern mathematics is this lesson: Whenever you have to do with a structure endowed entity Σ, try to determine its group of automorphisms, the group of those elementwise transformations which leave all structural relations undisturbed. You
can expect to gain a deep insight into the constitution of Σ in
this way. After that you may start to investigate symmetric
configurations of elements, i.e., configurations which are invariant
under a certain subgroup of the group of all automorphisms [...]
Weyl
It is a most beautiful and aweinspiring fact that all the fundamental laws of classical physics can be understood in terms of one mathematical construct called the action. It yields the classical equations of motion, and analysis of its invariances leads to quantities conserved in the course of the classical motion. In addition, as Dirac and Feynman have shown, the action acquires its full importance in quantum physics. Ramond
If we imagine a machine so constructed as to produce thought, sensation, perception, we may conceive it magnified — to such an extent that one might enter it like a mill. This being supposed, we should find in it on inspection only pieces which impel each other, but nothing which can explain a perception. It is in the simple substance, therefore, — not in the compound, or in the machinery, — that we must look for that phenomenon [...] Leibniz
Pythagoras could be called the first known string theorist. Pythagoras, an excellent lyre player, figured out the first known string physics — the harmonic relationship. Pythagoras realized that vibrating Lyre strings of equal tensions but different lengths would produce harmonious notes (i.e. middle C and high C) if the ratio of the lengths of the two strings were a whole number.
Many
of the foundations of wave mechanics are based on the analyses and
equations that Rayleigh
derived for the theory of acoustics in his book The Theory of Sound.
Erwin Schrödinger, a pioneer in quantum mechanics, studied this book
and was familiar with the perturbation methods it describes.
Masters
It
was not until the advent of quantum mechanics in the twentieth century
that absorbtion spectra were given a satisfactory theoretical
explanation. They were shown to correspond with eigenvalues of
appropriate Schrödinger operators. A given atom could absorb or emit
light only at certain frequencies, corresponding to the energy levels
of bound states represented by different eigenvalues. The mathematical
spectra of differential operators thus carried fundamental information
about the physical world, which even now seems almost magical. The analogy with number theory is through spectra of other differential operators. These are LaplaceBeltrami operators (and variants of higher degree) attached to certain Riemannian manifolds. The spectra of these and other operators are expected to carry fundamental information about the arithmetic world, a possibility that also seems quite magical. [...] The spectral data that is believed to be related to number theory is framed in the language of automorphic forms. Arthur
Like
the efforts of an Anton Chekhov character, Lobachevsky's effort to
disseminate his nonEuclidean geometry was utterly futile. He knew he
had invented something profoundly important, and he worked for years to
perfect and demonstrate its mathematical significance. The tragedy of
his life is that nobody listened.
§ Some call it the greatest revolution in mathematics since the time of the Greeks — the discovery that changed the definition of a straight line. In ordinary, flat, Euclidean geometry, a straight line is exactly that — its "straightness" defined by the singular unbending direction that it follows for its length. In nonEuclidean geometry, a straight line is defined simply by the fact that it joins two points within a given space. Straight lines may actually be curved. Janos Bolyai, who called himself Euclid's phoenix, defined absolute geometry as that form of geometry in which the theorems were true regardless of whether they were Euclidean or nonEuclidean. §
Klein
fully developed the idea of a general geometry as being about the
invariant properties of a group of defined transformations. His work
fundamentally advanced nonEuclidean geometry from a rigorous, if
fanciful, subject into something that was on equal footing with
Euclidean geometry. Klein also gave Gauss so much credit for non
Euclidean geometry that it would become his standard due.
§
Riemann
gave a lecture to his fellow faculty members at Gottingen on June 10,
1854, shortly before Gauss died. Riemann's these was titled "On the
Hypotheses Which Lie at the Basis of Geometry." Gauss attended the
lecture, which set in motion a change in mathematics that continues to
unfold today.
§ The most fundamental conceptual breakthrough Riemann made was to determine that bodies in a physical space are not simply occupants of this space but actors that bend and shape the space itself by their very presence. In doing so he anticipated the central concept and laid out the mathematical foundation of Einstein's general relativity theory by more than sixty years and even suggested that space could be measured by its physical masses. This insight was astounding considering that Riemann was a classical physicist working more than fifty years before the advent of relativity. Bardi









