The proposed Unified Field Theory (UFT) provides an
all-encompassing theory, where physical models of different physical areas are
no longer decoupled and differently scaled according to their different levels
of granularity, (BrK0) pp. 10-13. It is governed by two types of energy, the
today’s mechanical energy (i.e., the space-time based kinetic and potential energy)
and a newly proposed dynamic energy, which is timeless and spaceless. Bohm suggested a „wholeness, explicate &
implicate order" principle for quantum theory, (BoD). In this context the mechanical energy is about explicate momentum and explicate potential differences of particles in a space-time continuum, while the new dynamic energy is characterized by implicate potential differences modelled by indefinite norms (i.e., the invariances of the considered quanta systems) of appropriately defined Krein spaces.
There are two order-creating principles (or
mechanisms) in classical physics, the order-from-disorder principle (e.g. in
statistical thermodynamics), and the order-from-order principle
in classical dynamic laws (e.g. the Newton law, F = m*a), (ScE), (PlM).
Bohm suggested a „wholeness, explicate & implicate order"
principle for quantum theory, (BoD). The proposed Unified Field Theory
(UFT) provides a deductive dynamic system structure enabling an
order-from-order-creating principle starting from meta-physical (mathematical)
dynamic quanta systems up to Hilbert space based classical partial differential
equation (PDE) systems.
The scope of the Unified Field Theory (UFT)
includes the scope of the three quantum field theories of strong interactions, of weak interactions, and of electromagnetics), the Higgs mechanism, the scope of
both relativity theories, and plasma dynamics.
The variational
principles of mechanics are one of the most important concepts in mathemtical physics.
The related mathematical tool is the calculus of variations. The new conceptual
elements of the proposed deductive structure of physics are additional (Hilbert
space and Krein space based) bases layers. The current Hilbert space frameworks
of the calculus of variations become approximation Hilbert sub-spaces of an
extended new Hilbert space layer. This layer (building block 2) become an
approximation Hilbert space layer of underlying Krein space based layers. The central
differentiator between Hilbert and Krein spaces are definite vs. indefinite
norms. The central physical common denominator of Hilbert resp. Krein spaces are
underlying self-adjoint (mechanical resp. dynamic) operators. The central
physical differentiator between Hilbert resp. Krein space based frameworks are,
that the latter frameworks are without the concepts of space and time governed by the complex Lorentz transformation group.
The two linked mathematical frameworks: Krein & Hilbert scales
A Hilbert space framework may be considered as the only possible common
denominator of a GRT (based on the Hilbert-Einstein action functional) and
quantum mechanics. In a Hilbert space there is a definite (invariant) norm induced
by its inner product. The Krein space theory is basically the theory of linear
spaces with an indefinite metric. It provides the concept of an intrinsic
self-adjoint "potential" operator, which is defined by the so-called J-symmetric operator and related J-inner product on all of the considered Krein space, (BoJ) p. 120 ff.. This dynamical "Hamiltonian" operator is applied to define quantum type specific
"dynamic energy" inner products and corresponding dynamic quanta energy
systems, (BrK0) pp. 1, 27-29, 36.
It turns out that the Krein space based dynamic quanta
systems can be approximated by an energetical H(1/2) Hilbert space
framework. This Hilbert space includes the domain of the self-adjoint Friedrichs extension of
the (mechanical) symmetric Laplacian operator providing the concepts of a dynamic
fluid particleanda related (not self-adjoint) dynamic potential
operator, (BrK0) pp. 10, 11, 17-19, 38. However, this dynamic potential
operator can be interpreted as a compact disturbance of the mechanical (self-adjoint) Laplacian potential operator with domain H(1). It enables a convergent energy
norm estimate of the non-linear, non-stationary 3D-NSE system. It further
provides a modified Schrödinger 2.0 momentum operator. This is basically the Schrödinger operator in combination with the Riesz
operator: the Riesz operator commutes with translation and homothesis, and have nice properties relative to rotations. For n=1 the Riesz operator is called the Hilbert transform on R.
1. The current phenomenological & conceptual
structure of physics
There is a phenomenological and a conceptual structure of physics, which are
mutually dependent on each other. This results into regional disciplines of
physics, where physics at large scale decouples from the physics at a smaller
scale accompanied by different degrees of freedom and different dynamics:
In classical mechanics one deals with three scales according to its three basic
measurements: distance D, time T, mass M. In non-relativistic quantum theory
and classical relativity it has two scales: D & T resp. D & M (mass M
can be expressed through T & D using the Planck constant resp. T can be
expressed via D using the speed of light). In relativistic quantum theory there
is only one scale: distance D, (DeP) p. 551.
2. Challenges ... a. ... in current thermomechanics / thermodynamics Thermomechanics deals with thermal and mechanical
process (Brown motion). Thermodynamics dealing with the concepts of
temperature, pressure, and volume is governed by four principles, (1) thermal
equilibrium, (2) energy conservation, (3) entropy, (4) unattainable absolute
zero point. In all cases only closed energetical system are considered.
There is, essentially, only one problem in statistical
thermodynamics: to determine the distribution of an assembly of identical
systems over the possible states in which this assembly can find itself, given
that the energy of the assembly is a constant. The idea is that there is weak
interaction between them, so weak that one can speak of the „private“ energy of
every one of them and that the sum of their „private“ energies has to be equal
E. The distinguished role of the energy is, therefore, simply that it is a
constant of the motion – the one that always exists, and, in general, the only
one, (ScE) pp. 1-2.
b. ... in current quantum mechanics / quantum dynamics
Quantum mechanics is concerned with states and process
of matter. Quantum dynamics is concerned with motions and interactions of closed
quantum systems over time. Aditionally to matter it deals with the concept of
fields. Accordingly, there are decoupled matter and interaction objects
(fermions & bosons)
for each quantum dynamic phenomenon or modelling case (QED
(interaction between matter and light), QCD, QFD, Higgs). The three SMEP
systems show similar gauge symmetry properties. The Higgs system is incompatible
with the SMEP systems. c. ... in current galactic
mechanics / galactic dynamics There seems to be no clear differentiation between galactic
mechanics and galactic dynamics. Most probably, because there is no closed system to
be considered. A similar unspecified situation exists in case of all „theories“
based on the so-called Big Bang „Theory“ („even though it was the biggest black
hole ever, it exploded out of nowhere“, (DeK); „producing an universe
resembling the one in which we live with a probability of the inverse of 10
exp (10 exp (123))“, (PeR) p. 444). The probability that God made it within six days including a beer to celebrate the work at the seventh day seems to be more likely, especially as this scenario provides also an explanation of the existence of organisms on Earth. In any case, the most mathematical tool being
applied so far in galactic dynamics are ordinary differential equations depending from a „cosmic time“ parameter and a few cosmic constants like the Hubble constant.
Galactic (stellar) dynamics is the principle tool for
the study of the motion of a large number of point masses orbiting under the
influence of their mutual self-gravity, (BiJ) xiv. In its purest form, Landau
damping represents a phase-space behavior peculiar to collisionless systems. The
dynamic plasma characteric, the Landau damping also exist in the interactions
of stars in a galaxy at the Lindblad resonances of a spiral downsity wave. Such
resonances in an inhomogeneous medium can produce wave absorption (in space
rather than in time), which does not usually happen in fluid systems in the absence
of dissipative forces (an exception in the behavior of corotation resonances
for density waves in a gaseous medium), (ShF) p. 402.