After almost 3 years of silence -while I was like the mouse in the cage, wheeling around without getting anywhere, here is something new announcing that finally I found something that looks like the combinatorial equivalent of a Pseudo-Riemann Differential Manifolds.
It appears as if all boiled down to find the most appropriate universe of discourse to name the abstract objects I was struggling with.
Here is the story:
Name it – tame it
When creating new Mathematics -new structures,
properties, relations and operations- sooner or later you face a non-mathematical
but non-trivial problem: how to name them.
If you use already established names, obviously
you have to show that your objects belong to the same category of objects
already baptized or at least to the same family that is sharing some typical
characteristics while dropping or generalizing others, else an already
familiarized reader would be misled intuitively into wrong assumptions and
worse false conclusions.
The most radical approach would be to invent
the names themselves that is even new words as sequences of letters that never
have been used before. Yet words in common language do not come isolated but as
a vocabulary belonging to some common problem domain, a for that problem
domain.
Much of Mathematics itself consists in taking some
of these words as terms defining their initial meaning that is converting
intuition by means of axioms into Mathematics, and then proceeds to derive
properties, relations and operations using the tools of mathematical logic
while preserving o précising the intuitive meaning of the corresponding term in
the original vocabulary.
Geometry itself is a mathematical subject,
which started in the Euclidian Geometry using some terms of the Anschaung as still informally defined
axioms yet a rigorous argumentation-scheme to derive properties, relations and
operations.
It’s formalization starting the early XIX
century did not only provide us with new types of geometries, not covered by
Euclid himself, but finally with an extremely powerful mathematical tool,
Differential Manifolds, which is right at the heart of General Relativity as we
know it now.
However in this context Sheaf-theory shows another way Mathematics adopts common
language terminology not as only
isolated words but as a vocabulary of meaning-connected words. Here
the imported vocabulary itself is not the object of study but serves or at
least aims to serve as an intuitive guidance to comprehend the otherwise
completely abstract, purely mathematical structures. I do suspect it was even more
and earlier: the imported language served as mind-guidance to its creators
while creating the new theory itself.
At its beginning, the mathematical language for
General Relativity that Einstein used was Tensor-Calculus, which in turn was
developed during the XIX century starting with Gauss. Its real problem-domain
was literally Geometry not as an
abstract mathematical subject but as a technology used to create the first
large-scale exact maps. As the areas were by far greater than Attica, pure
Euclidian Geometry and its algebraization by Descartes were insufficient as
they did not take into account the curvature of earth. Hence much of the new
names for the new mathematical objects were an import from the language of the
land-surveyors.
The now most frequently used
mathematical language for advanced GRT is the Calculus of Differential Forms as
developed by Cartan at the beginning of the XX century. While maintaining
Differential Manifolds as a fundamental concept, the Cartan Formalism provides
a concise yet very compact hence very elegant language to express complicated
relations, yet its full theoretical background includes many concepts from many
areas, from Topology to Lie-Groups. That’s sufficient stuff to fill a complete
curriculum for postgraduate studies in Mathematics. Therefore most introductory
courses into GRT still rely on the original Tensor-Calculus. Yet on the other
hand almost all attempts aimed at Quantum-Gravitation start with the
Einstein-Cartan form of GRT.
GRT as such combines two rather
different concepts: Causality and its
rules as defined by Special Relativity
and Gravity as modification of the
space-time geometry, both connected by Einstein’s field equitation, where -as John
Archibald Wheeler put it- "Space-time tells matter how to move; matter
tells space-time how to curve."
A closer look on Causality first by Stephen Hawking then
by David B. Malament moreover revealed that it comes with its own geometry,
named causal structure, whose topology is somewhat related yet not equivalent
neither to the topology created by gravity nor the topology of the underlying
Differential Manifold. Similar, the effects of Gravity can be completely described by the geodetics of free
falling particles, which are both causal
paths w.r.t. Causality and extremal paths w.r.t. Gravity. Seen as Geometries, the first correspond to conformal Geometry, the latter to projective Geometry, which together completely define a
Pseudo-Riemann Differential Manifold.
The concepts and tools provided by
the above 2 structures are not sufficient to express neither of Einstein’s
famous equations i.e. neither E = M c2 of SRT nor the Field equation
of GRT. Worse yet they do not allow to express the special equivalence principle i.e. inertial mass = gravitating mass,
leaving it buried inside the formalism of Tensor-Calculus; the more general
idea that Physics is the same – anywhere,
anytime degenerates into covariance, which was meant by Einstein as an
expression for the former not it’s founding.
While it’s rather straightforward to
find combinatorial structures to model Causality and the effects of Gravity,
actually the causal-structural itself is a combinatorial structure, it turned
out to be quite difficult to find an combinatorial substitute for the
Differential Manifold itself and its construction and almost impossible in the
vocabulary of surveyor’s geometry
where the constituents are just maps,
alas descriptions. It’s already almost impossible to grasp using this
vocabulary the conceptual difference between active and passive
Diffeomorphisms as introduced by Carlos Rovelli. Yet without that
substitute there is no way neither to find a combinatorial substitute for the
Cartan Formalism, even if the latter already eliminated algebraic invariance
using geometrical symmetry instead. And without that substitute there is, in my
humble understanding, no Quantum-Gravity either.
May be due to my laziness –I did not
invest the equivalent of a postgrad-curriculum- may be due to my other
limitations, I made countable many attempts to find this substitute, always
staying within the traditional
vocabulary for Differential Manifolds. Finally I decided to drop this
vocabulary all together and to switch to another taken from textiles. Now everything fits neatly, at
least up to the combinatorial equivalent of a Pseudo-Riemann Differential
Manifold, yet still –and fortunately- without metric.
As mathematical structure beneath we use connected locally
path-connected Topologies, yet weaker
than the usual Haussdorff-Space of Differential Manifolds. Our category of
topologies includes discrete models, alas Petri-Nets. What in the Haussdorff
case are the paths of Jordan-Curves is generalized into ropes.
In my framework for new terminology,
you may think about Einstein’s Universe
as a patchwork of many fabric pieces, tied together by compatible seams. The seaming process and its compatibility condition resemble the
classical construction of a Differential Manifold. Even more: using proper strands that is subsets of ropes -the paths of continuously
differentiable Jordan-Curves- and specific seams -patch-wise isomorphic- the
resulting quilt is the combinatorial equivalent of a Differential Manifold.
Classical fabric is made out of 2 quite different components, the warp and the weft, where
the warp defines a fixed, pre-tensed setting that the weft may transverse connecting;
or catching up Wheeler, warps will resemble effects of Gravity, wefts
Causality. A weaving process puts
both together, where shedding is
formally expressed by strands that belong to both structures, as were the
geodetics of free falling particles.
As a result, using the above
mentioned proper strands and specific seams, the woven fabric is the
combinatorial equivalent of a Pseudo-Riemann Differential Manifold yet without
metric.
Up to here the ideas are completed (to follow soon).