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Appendix B
UNITARY FIELD THEORY
AND QUANTUM GRAVITY
B.1. The process of unification in physics
B.2. Einstein's
visions of geometric unitary field theory
B.3. Wheeler's
geometrodynamics. Gravity and
topology.
B.4. Quantum geometrodynamics
B.5. Gravitational
field quantization
B.6. Unification
of fundamental interactions. Supergravity.
Superstrings.
B.7. General
principles and perspectives of unitary field theory
B.4. Quantum geometrodynamics
To recap, the geometrodynamic view of the world of classical (non-quantum) physics is admirably uniform: there is nothing but empty space-time , all matter, fields, and charges are a manifestation of the geometric and topological properties of empty space. Classical physics could thus be fully unitarianized.
However, we know that
nature is much more diverse - more than 300 types of
"elementary" particles are known, the charge is
quantized, etc. Geons with their large mass and overall classical
structure cannot be directly related to elementary particles,
similar to geometrodynamic electric charges arising in a curved a
multiply connected space are not directly related to quantum n ym
charges of elementary particles. From this point of view, the
whole classical geometrodynamics appears only as an interesting
physical-mathematical prank.
To harmonize geometrodynamics with the world of elementary particles^{ }it would be possible to try to
implant appropriate quantum fields (meson, neutrino, etc.) into
"pure" geometrodynamics. Then it would be necessary to
introduce appropriate phenomenological coupling constants and
would appear other shortcomings of the existing apparatus of
quantum field theory (difficulty renormalizations), so that in
fact the ytratily appealing features
geometrodynamiky a perfectly unitary theory.
^{ }Wheeler went a different way: he
tried a quantum formulation of his classical geometrodynamics in
the hope that the resulting quantum
geometrodynamics
could explain the properties of elementary particles. In other
words, he investigated the consequences of quantum
uncertainty relations in geometrodynamics.
Quantum
field fluctuations and space-time geometry
The basic postulate of quantum mechanics is the well-known
Heisenberg uncertainty principle D x. D p ³ h , where h º h / 2 p @ 1,05.10
^{-27} g cm^{3}/s is the Planck constant. The
relation of deafness D A. D B ³ h
holds between every
two dynamically coupled quantities A and B ; for example
size A: | size B: | |
position x | ç ----- no | momentum p |
time t | ç ----- no | energy E |
electric field strength E |
ç ----- no | magnetic field strength B |
internal curvature of space | ç ----- no | external curvature of space |
If we observe, for example, a magnetic field in a small spatial region characterized by the dimension L, there will be energy proportional to B ^{2} .L ^{3} and the time required to measure the field will be L / c; uncertainty relation D E. D t ³ h then gives ( D B) ^{2} .L ^{4} ³ h .c, or D B ³ h c / L ^{2} . We can say that quantum fluctuations of the electromagnetic field in size L , they are about equal
D E ~ D B ~ D A ^{i} ~ Ö ( h .c) / L ^{2} . | (B.8) |
Thus, the field is constantly "oscillating" between configurations whose fluctuation range is greater the smaller the spatial areas we observe. Effect of these quantum fluctuation of the motion of the electron around the atomic nucleus is shown schematically fig.B.5 (these quantum fluctuation "overlap" Broglie waves through the Bohr model of the atom - see " Bohr model of the atom " in §1.1 " Atoms and atomic nuclei "monograph" Nuclear physics and physics of ionizing radiation ", fig.1.1.6) .
Fig.B.5. Schematic representation of the motion of an electron around an atomic nucleus. A closer look at the Kepler trajectory of the electron would reveal the chaotic irregularities caused by quantum fluctuations in the electric field. The mean deviation from the global trajectory is zero, but the mean square deviation leads to a small shift in the energy level. This shift was actually measured as part of the Lamb-Rutheford shift. |
Assuming the universal validity of the quantum uncertainty principle, a similar situation must occur in geometrodynamics: quantum fluctuations in the space-time geometry will manifest themselves . In the spatial region with characteristic L dimensions (investigated in a locally inertial system with diagonal metric coefficients -1,1,1,1), the fluctuations of the space-time geometry, ie metrics, connections and curvatures, will be of the order of equal
D g _{ik} ~ L * / L, DG ^{l }_{ik} ~ L * / L ^{2} , D R ^{i }_{klm} ~ L * / L ^{3} , | (B.9) |
where
L * = Ö ( h .G / c ^{3} ) @ 1.6. 10 ^{-33} cm | (B.10) |
is the so-called Planck-Wheeler length , which was formally introduced as early as 1899 by M. Planck and whose fundamental significance was clarified by J.A.Wheeler in 1955.
Fluctuations
in geometry and topology of spacetime
In the scales L » 10 ^{-8} cm, with which atomic physics
works, D g ~ 10 ^{-25} ; even for the scales L » 10 ^{-13} cm of nuclear physics, the
quantum fluctuations of the metric D g » 10^{-20 }are
completely negligible. Therefore, in all the situations we face
so far, we can rightly consider space-time as a smooth continuum . Of marital positively postulate of classical
(non-quantum) physics - special and general theories of
relativity that space is locally Euclidean, is very well
satisfied.
Fig.B.6. At very small scales, the spontaneous quantum
fluctuations of space metrics increase ( a , b ). In the area of ??Planck lengths, these
fluctuations may eventually increase to such an extent that the
space becomes multiple contiguous ( c ) - they grow into bizarre fluctuations in
the topology (enlarged sections in Fig. D ).
However, if we go to ever smaller scales (Fig. B.6a, b), quantum fluctuations gradually increase, only in areas of size L » 10 ^{-33} cm, where according to (B.9) D g ~ 1, the fluctuations of the metric already so strong that the overgrowth melts in topology fluctuations - Fig.B.6c, d. The dynamic evolution of curved empty space in connection with the quantum principle thus leads to specific laws at very small distances: in microscales of the order of ~ 10 ^{-33} cm not only the geometry but also the topology of space fluctuates very strongly ( D g » 1).
From a normal point of
view, spacetime appears to us as a continuous smooth continuum.
Similarly, when we look at the surface of the ocean from a
high-flying plane, we see a completely smooth surface, only
slightly globally curved (in the shape of a globe) - Fig.B.7a. If
the observer jumps with a parachute and gradually approaches the
surface, he can see more and more clearly that it is rippled
(Fig.B.7b). When he finally lands on the water with a rubber
dinghy, he realizes how far the surface is to an perfectly flat
and smooth surface - the surface ripples sharply, spraying foam.
^{ }In meter scales, the local
curvature of the surface (waves) fluctuates strongly, in
centimeter and millimeter scales even the topological structure
of the surface fluctuates - drops separate, foam bubbles are
formed (Fig.B.7c).
^{ }
Fig.B.7. The analogy between the geometric-topological structure
of spacetime and the structure of the ocean surface .
a ) When viewed
from a height of several kilometers, the sea level appears to be
an ideally smooth surface.
b ) From a height
of several tens of meters, the surface appears wavy, but
otherwise smooth.
c ) It can
be seen from the immediate vicinity that not only the curvature
of the surface, but also its topological structure (bubbles,
drops) fluctuates strongly.
Similarly, in our
spatiotemporal "continuum" the smaller the microareas we observe, the more pronounced the quantum fluctuations
of the geometry will be manifested, until finally the space
topology itself will fluctuate strongly in the Planck length l _{p} » 10 ^{-33} cm. For example, topological
tunnels will be formed and destroyed, closed areas will be
created (virtual "black
microdires" that will evaporate immediately quantum - see
§4.7 " Quantum radiation and thermodynamics of black
holes ") , even new "microvirms"
("bubbles" can be separated ) . "which
then disappear; but with random fluctuations of sufficient
magnitude, they are likely to expand in inflation and
the emergence of a "new" macroscopic
"universe" - §5.5, part " Chaotic inflation and quantum cosmology ", passage " The
emergence of more universes
") . According
to quantum geometrodynamics, therefore, this seemingly empty
vacuum is the scene of the most turbulent microevents - spacetime
has a kind of " foamy " constantly spontaneously
fluctuating microstructure .
^{ }If an idealized point *) test
particle enters such a place, it will be mercilessly slid
left-right, up-down, and chaotically here and there in all
directions, until it loses any idea of ??temporal sequence and
spatial proportions — space and time cease to exist for
it .
*) If the test particle had non-zero
dimensions, it would be immediately torn apart by fluctuating
tidal forces.
Quantum fluctuations of
spacetime: reality, or maybe forever just a hypothesis?
To some extent, by formally combining the laws of quantum physics
and general theory of relativity, it can be concluded that in
areas smaller than Planck's length » 10 ^{-33} cm, quantum vacuum fluctuations are so
large that not only the geometry fluctuates, but also spacetime
topology - spacetime here "boils" like a bubbling
" quantum foam ". In these Planck-Wheeler
microscales, quantum foam is ubiquitous : it is not only in
singularities inside black holes, but also in interstellar space,
around us, inside the cells of our brain, inside atomic nuclei
and particles. Under normal conditions, however, the
quantum fluctuations of the spacetime metric are so slight that no experiment has yet revealed them.
To "see" them, we would have to have a hypothetical
" supermicroscope " providing a magnification
of » 10 ^{-32} times and higher *).
*) A more high-quality optical microscope
is able to provide a maximum magnification of about 3.10 ^{3} times. The
fundamental limitation here is given by the wavelength of visible
light. The electron microscope can give a magnification of up to » 10 ^{5} -´. Tunneling
microscopes and electrostatic microscopes are under development,
which will make it possible to image even heavier atoms. However,
it is unimaginably far from Planck's details!
^{ }If we on the imaginary virtual
experiments on this "supermikroskopu" gradually
increased magnification on »
10 ^{8} ' , we observed atoms at a magnification » 10 ^{13} ' would be able to
"see" the atomic nuclei, the nucleons and quarks inside
them. But even with further growth of magnification, the space
would remain completely smooth, with only a slight continuous
curvature given the gravitational mass. Only if we increased the
magnification by another incredible 20 orders of magnitude to see
the dimensions » 10 ^{-32}cm, we would first observe small,
but gradually larger and larger fluctuations in the curvature of
space. And at a magnification of about 10 ^{33} times, the space would resemble bubbling
stochastic-quantum "foam" (Fig.B.6d).
^{ }Directly achieving such an increase
is of course impossible not only for technical,
but mainly for principal (quantum-physical) reasons. Even complex
and ingenious indirect experiments will not be able to prove
quantum fluctuations of space-time in the foreseeable future (but see the following passage on the possible influence
of quantum fluctuations of space on the speed of high-energy
photons ...) . They will remain for a long
time (maybe forever?) Only at the level of an interesting hypothesis
..! ..
Possible practical
consequence :
Is
high-energy g- radiation moving slower than light
?
All electromagnetic radiation propagates in a vacuum at exactly
the speed of light c , independent of the movement of the
source and the observer. This is a basic finding, firmly rooted
in the special theory of relativity. Regardless of the wavelength
- speed c propagates radio waves, visible light *), X and
gamma radiation. *) The classical
dispersion, observed with light in the matter's optical
environment, originates in the (collective) interactions of the
electromagnetic wave with the atoms of matter; does not occur in
a vacuum.
Fig.B.7d) Influence of quantum micro-fluctuations of space-time
geometry on the speed of motion of high-energy photons of gamma
radiation.
However, in connection with the mentioned quantum-gravitational
fluctuations of spacetime , there may be phenomena that
may call this basic initial statement of the special theory of
relativity into question in certain circumstances *). Fig. B.7.d
shows a situation where two photons are emitted from a certain
source at the same time: one photon with a lower energy, ie a
longer wavelength, the other photon of high-energy gamma
radiation with a very short wavelength. For radiation with a
longer wavelength, the quantum fluctuations of the metrics are
averaged and completely smoothed out in the respective longer
scale, so that this radiation will move exactly in the classical
vacuum at the speed of light v = c. Photons of high-energy
radiation ghowever, with a very short wavelength, they will be
"more sensitive" to fine-time fluctuations in
space-time metrics than low-energy photons. Such waves will move
along a slightly undulating geodetic orbit, photons will in a
sense "penetrate" the unevenness of the orbit, caused
by subtle metric perturbations, and their effective velocity v _{ef} will be slightly less
than c . Locally, such a photon travels a slightly longer
trajectory than would correspond to a smooth space. We can
compare this to the movement of a car with small wheels and large
wheels on a bumpy road: when driving the wheels at the same
circumferential speed, a car with small wheels (copying a bumpy surface) will
drive a little slower than a car with a large wheel diameter(whose circumference extends beyond small depressions) .
* ) This is not
considered a breach or failure of the special theory of
relativity, which applies exactly flat spacetime metric defect
free (eventual in locally inertial system GTR) ..
^{ }These differences in propagation
speed are reflected only at the very high energy
radiation g , in the field of GeV and TeV. Here, too, the
differences in speed are very small (of the order of 10 ^{-20} ), without the
possibility of laboratory measurements. In the future, they could
only be demonstrated by a temporal comparison of the detection of
light and flashes of hard g-radiation from catastrophic processes in outer space.
At cosmological distances of billions of light-years, even these
slight differences in speed could "accumulate" and have
measurable effects (the problem, however, is to distinguish these
differences from the differences in emission times in the sources
themselves ...).
^{ }Interactions with
quantum-gravitational fluctuations of space can lead to
dissipative phenomena and a slight modification of the
kinematics not only of hard photon radiation, but also
of high-energy particles in space.
Huge quantum
microfluctuations
Quantum fluctuations cause the space to have, in addition to
macroscopic (gravitational, cosmic) curvature, also
"microcurvature" of radius of the order of L * » 10 ^{-33} cm and that the necks of
topological tunnels are formed everywhere, whose dimensions and
mutual distances are also of the order of ~ L * . If we have a
topological tunnel of size L (and thus areas ~ L ^{2}
), there will be quantum fluctuations of electric field intensity
of the order of Ö ( h c)
/ L ^{2} , so that the total field strength flow
indicating the effective electric charge will be of order of q ~ Ö ( h . c) » 10.e, regardless of the dimensions of the
tunnel. The typical charge in geometrodynamice but not directly
related sn s struggle elementary particles because it
is an order of magnitude greater than the bounty elementary
charge e and not quantized. The energy density E ^{2}
/8 P field in a typical tunnel reaches enormous
values ~ H C / L * ^{4} » 5.10 ^{93} g / cm ^{3} and characterized by mass-energy
per one topological tunnel makes m ~ Ö ( h .c / G) @ 2.2.10
^{-5} g » 10 ^{19}GeV, which is at least 20 orders
of magnitude more than the rest mass of elementary particles (and
about 9 orders of magnitude more than the maximum energy
registered in cosmic rays).
^{ }These huge values are obviously at odds with the very low mean energy density
that we observe in space. However, if we take into account the
contribution of gravity to the density of energy and mass, then
two typical tunnel mouths with masses m _{1} » m _{2} ~ Ö ( h c / G) = ~ 10 ^{-5} g, spaced r _{1,2} » L* @ 10 ^{-33} cm, will have a binding energy E
_{gr} = -Gm _{1} during mutual gravitational
interaction^{ } m _{2} / r _{1,2} » -c ^{2} Ö ( h c
/ G). Mass defect of two adjacent mouths of topological tunnels D m _{gr} = E _{gr} / c ^{2} ~ - Ö ( h c / G) @ -10 ^{-5} g, which is negative and of the same
order as the (positive) electromagnetic mass of both structures,
can therefore locally to compensate
for the
energies of the respective fluctuations. Such locally compensated
fluctuations no longer show gravitational attraction with more
distant concentrations of matter and energy. After such a total
compensation of the huge picofluctuations, the vacuum may look as
if we observe it.
^{ }However, the observed elementary
particles, which are probably not far from elementary, have
dimensions of the order of 10 ^{20} times larger than the Planck
length, and thus could perhaps be a kind of "collective
excitations" (involving a large number of elementary
fluctuations ) in a sea of strong microgeometry
fluctuations. everywhere else it cancels on average and
macroscopically creates the usual "vacuum". Whether
this is the case and how it is going, no one knows yet ...
Micro
fundamental values of physical quantities
Therefore, even though the quantum geometrodynamice far failed to
explain the structure of el ementárních particles provides
important limit fundamental values of some basic physical
quantities :
l _{p} º L * = Ö ( h .G / c ^{3} ) @ 1.6. 10 ^{-33} cm | - Planck length | (B.11) |
t _{p} º t * = L * / c @ 10 ^{-43} s | - Planck's time | |
m _{p} º m * = Ö ( h .c / G) @ 2.2. 10 ^{-5} g | - Planck's mass |
Quantum spacetime
structure here shows that a smaller distance than L * » 10 ^{-33} cm shorter than the time
intervals t * » 10 ^{-43} of no significance because the spatial
relations and time relations are due to quantum fluctuation
topology pointless. From a quantum point of view, space and time
are not a continuous infinitely divisible continuum,
but effectively have a "grainy" discrete
structure of
some "atoms" or "elementary particles" of
space and time - it decays into elementary Planck lengths ("
quantum of space ") and
Planck times ( " quantum of time ", also
sometimes called chronons ).
^{ }From the point of
view of nuclear physics, the issues of continuous or discrete
internal structure of space and time are discussed in the passage
" Is the world
continuous or discrete at the deepest level? " §1.1 of the book " Nuclear
Physics and Physics of Ionizing Radiation ".
^{ }We can imagine the following illustrative
justification for the smallest possible length: Visual
resolution of two nearby points in space requires the use of a
wavelength of light shorter than the distance of the points. The
energy of photons is inversely proportional to the wavelength, so
the closer the points are, the more photon energy we need.
According to OTR, this photon energy causes the curvature of
spacetime. At Planck's distance » 10 ^{-33} cm^{ }the curvature of spacetime (caused by the necessary
high-energy photons) would increase so much that the points would
be inside the horizon of a (virtual) black hole - measuring such
a small distance becomes fundamentally impossible
, spacetime is no longer continuous here. At the Planck length,
the GTR expires, and the physical processes are controlled by the
quantum theory of gravity (§B.5 " Quantization of the gravitational
field ") . Quantum geometrodynamics suggests that in the smallest
microscales there is a kind of " quantum of space
" on the background of a general variety without a metric
structure, space can be likened to "quantum foam". This
idea could be important for quantum field theoryin
general, since the energy of the quanta is inversely proportional
to the wavelength of the respective "wave ball". If the
wavelengths cannot be less than a certain lower limit (in our
case » 10 ^{-33} cm), because a shorter length
simply does not exist, then the energy
of the quanta is limited from above - quanta with infinite energy, which
causes such problems in quantum field theories, are in advance
excluded.
^{ }Planck-Wheeler units are natural
units for the description and modeling of natural laws based on
the properties of spacetime. The fact that there is the shortest length and shortest
time interval in space and time , about which it still
makes sense to talk about, is a knowledge that is beyond the
scope of geometrodynamics and perhaps even the whole of physics!
^{ }
Gravity, black holes and space-time physics : | ||
Gravity in physics | General theory of relativity | Geometry and topology |
Black holes | Relativistic cosmology | Unitary field theory |
Anthropic principle or cosmic God | ||
Nuclear physics and physics of ionizing radiation | ||
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