Open issues in physics in 2000Requirements for a final theoryPredictionsEnjoying physicsBetting
If you enjoy playing with ideas and then checking them against the real
world, you might like the following proposal for the final theory of
physics. The colour pdf file with embedded animations is free. If you
prefer a paper version in black an white delivered to your home,
click on paper
volume VI.
| 1 | From millennium physics to unification | 17 |
| 2 | Physics in limit statements | 22 |
| 3 | General relativity versus quantum theory | 48 |
| 4 | Does matter differ from vacuum? | 54 |
| 5 | What is the difference between the universe and nothing? | 77 |
| 6 | The physics of love - an intermediate report | 100 |
| 7 | The shape of points - extension in nature | 110 |
| 8 | The basis of the strand model | 142 |
| 9 | Quantum theory of matter deduced from strands | 158 |
| 10 | Gauge interactions deduced from strands | 197 |
| 11 | General relativity deduced from strands | 236 |
| 12 | Particles and their properties deduced from strands | 261 |
| 13 | The top of the mountain | 308 |
The pdf file presents an approach to the unified and final theory of physics
with a simple basis but intriguing implications. The model is based on
featureless strands and sums up textbook physics in a single
postulate: events and Planck units are crossing switches of strands.
Surprisingly, this postulate allows to deduce Dirac's equation (from the
belt trick), the principles of thermodynamics, and Einstein's field
equations (from the thermodynamics of strands). They all follow as
low-energy approximations of processes at the Planck scale. In particular,
strands explain the entropy of black holes.
As a further surprise, in the same approximation, the postulate yields the three gauge groups and the Lagrangians of quantum electrodynamics, of the strong and of the weak interaction, including maximal parity violation and SU(2) breaking. The Lagrangians appear as a natural consequence of the three Reidemeister moves. The strand model does not permit any further interaction, gauge group or symmetry group.
As a final surprise, the postulate predicts three fermion generations and the lack of any unknown elementary particles. The strand model thus predicts that the standard model, with slight corrections for longitudinal W and Z boson scattering, is the final description of particle physics.
A natural method for the calculation of coupling constants, particle masses and mixing angles appears. Mass sequences, some mass ratios and the weak mixing angle are predicted correctly.
The first seven chapters of the text deduce the requirements that any unified and final theory must fulfill. The strand model seems to satisfy each of the requirements. In particular, the strand model is based on Planck units, uses neither continuity nor discreteness as fundamental concepts, and does not assume that points or sets exist at Planck scale. The model has no free parameters, seems to be unique, seems to be unmodifiable, and works in three spatial dimensions. However, dimensionality is not a parameter, but a result of the model: other numbers of dimensions are impossible. The strand model also fulfils a famous wish: it fits on a T-shirt.
Additional points are found on the page on clear teaching and the page on fundamental research. Discussions about the strand model are possible on the fun discussion wiki.
Open issues in fundamental physics in the year 2000: the millennium list
This is the full list of questions that were unsolved in fundamental physics in the year 2000, the so-called millennium list of open issues. A unified and final description of nature must solve all these questions. Many such lists are found in the research literature; they are all contained in this one.
| OBSERVABLE | PROPERTY UNEXPLAINED IN THE YEAR 2000 |
| α | 1/137.0359991(1), the low energy value of the electromagnetic coupling constant |
| αw (or θw) | the low energy value of the weak coupling constant (or of the weak mixing angle) |
| αs, θCP | the value of the strong coupling constant at one specific energy value and the strong CP violation parameter |
| mq | the values of the 6 quark masses |
| ml | the values of 6 lepton masses |
| mW | the value of the mass of the W vector boson |
| mH | the value of the mass of the scalar Higgs boson |
| θ12, θ13, θ23 | the value of the three quark mixing angles |
| δ | the value of the CP violating phase for quarks |
| θ'12, θ'13, θ'23 | the value of the three neutrino mixing angles |
| δ', α1, α2 | the value of the three CP violating phases for neutrinos |
| 3 x 4 | the number of fermion generations and of particles in each generation |
| J, P, C, etc. | the origin of all quantum numbers of each fermion and each boson |
| c, ħ, k | the origin of the invariant Planck units of quantum field theory |
| 3+1 | the number of dimensions of physical space and time |
| SO(3,1) | the origin of Lorentz and Poincaré symmetry (i.e., of spin, position, energy, momentum) |
| S(n) | the origin of particle identity, i.e., of permutation symmetry |
| U(1) | the origin of the electromagnetic gauge group (i.e., of the quantization of electric charge, as well as the vanishing of magnetic charge) |
| SU(2) | the origin of weak interaction gauge group and its breaking |
| SU(3) | the origin of strong interaction gauge group |
| Ren. group | the origin of renormalization properties |
| δW = 0 | the origin of wave functions and of the least action principle in quantum theory |
| W = ∫LSM dt | the origin of the Lagrangian of the standard model of particle physics |
| 0 | the observed flatness, i.e., vanishing curvature, of the universe |
| 1.2 ⋅ 1026 m | the distance of the horizon, i.e., the ‘size’ of the universe |
| ρde = Λc4/(8πG) ≈ 0.5 nJ/m3 | the value and nature of the observed vacuum energy density, dark energy or cosmological constant |
| (5 ± 4) x 1079 | the number of baryons in the universe, i.e., the average visible matter density in the universe |
| f0(1, ..., c. 1090) | the initial conditions for c. 1090 particle fields in the universe (if or as long as they make sense), including the homogeneity and isotropy of matter distribution, and the density fluctuations at the origin of galaxies |
| ρdm | the density and nature of dark matter |
| c, G | the origin of the invariant Planck units of general relativity |
| δ∫LGR dt | the origin of curvature, of the least action principle and of the Lagrangian of general relativity |
| R × S3 | the observed topology of the universe |
As shown in the sixth volume of the Motion Mountain text, the strand model proposes an answer to each of these open issues. Each answer follows unambiguously from the single, basic postulate that strand crossing switches define the Planck units.
Requirements for a final theory
Any final theory must fulfil certain requirements. The list of requirements is rarely found or discussed.
The first half of the sixth volume shows how each requirement follows from the expression for the Compton wavelength and for the Schwarzschild radius. In other words, each requirement appears when quantum physics and general relativity are combined. None of the requirements follows from one theory alone. Thus, the search for unification is difficult because each requirement contradicts quantum physics and also contradicts general relativity. In a sense, each requirement for the final theory contradicts each part of 20th century physics.
The second half of the text shows that the strand model fulfils all these requirements. In fact, the strand model is the only present candidate for a final theory that fulfils them.
Some predictions of the strand model, all made before conclusive experiments (at the LHC, on neutrinos, on electric dipole moments, about QCD, on dark matter searches, and in astrophysics):
Enjoying physics
The final theory on a T-shirt? Yes. The search for unification is fun - and a beautiful adventure. One encounters many unexpected wonders of nature. Enjoy the reading!
Betting against the strand model
Do you want even more fun? Following European legislation, even many private bets must be agreed upon outside the internet. Following these laws, many bets are chance games. On the other hand, the validity of the strand model does not depend on chance. If you are convinced that the Higgs exists, that supersymmetric particles exist, that yet unknown elementary particles exist, that dark matter contradicts the standard model, that large electric dipole moments exist or that some other aspect of the strand model is wrong, email me at christoph@motionmountain.net.