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Thursday, December 27, 2012

Firewall mania

Multiverse mania has transformed to firewall mania. The posting of Peter Woit explains sociological background and gives a lot of links to articles about the newest fashion of the declining theoretical physics.

The 28 years of superstring models have led us to where we started from. The work with M-theory landscape is not very rewarding, and it is much sexier to produce wordy arguments about black-hole firewall. There are a lot heated debates and many conferences can be organized. Few years will pass until some new buzzword pops up and firewalls are forgotten. "Mountains are giving birth to mouse" as the text book of Latin from my school days expressed it.

I have said this many times earlier but repeat it: It would be really a high time to make questions about fundamentals. What happens in the interior of black holes? How the theory of general relativity could be modified to get free of its singularities and from its problems with the basic conservation laws? Could we generalize super string models to get 4-D space-time in natural manner out of the theory?

We refuse to do this because we have decided that M-theory is the final answer, and we refuse to consider the possibility that these nice formulas for black-hole entropy which we cannot test empirically might have nothing to do with reality. Somehow just those beliefs which are not testable are always the strongest ones. A related observation: the most noisy advocates of superstrings seem to do nothing to develop it! Perhaps this is natural, healthy laziness deriving from sub-conscious knowledge of the sad truth.

I have never been accepted to the "circles" so that I have not felt the social pressure of fashion, and have been free to develop an approach providing answers to the questions stated above and to many others too. I do not wish to retype what I have already written so that I give a link to the earlier blog article Do blackholes and blackhole evaporation have TGD counterparts?.

Wednesday, December 26, 2012

Particle physics Christmas rumor

We are not protected against particle physics rumors even during Christmas. This time the rumor was launched from the comment section of Peter Woit's blog and soon propagated to the blogs of Lubos and Phil Gibbs.

The rumor says that ATLAS has observed 5 sigma excess of like sign di-muon events. This would suggests a resonance with charge +/- 2 and muon number two. In the 3-triplet SUSY model there is a Higgs with charge 2 but the lower limit for its mass is already now around 300-400 GeV. Rumors are usually just rumors and at this time the most plausible interpretation is as a nasty joke intended to spoil the Christmas of phenomenologists. Lubos however represents a graph from a publication of ATLAS based on 2011 data giving a slight support for the rumor. The experiences during last years give strong reasons to believe that statistical fluctuation is in question. Despite this the temptation to find some explanation is irresistible.

TGD view about color allows charge 2 leptomesons

TGD color differs from that of other unified theories in the sense that colored states correspond to color partial waves in CP2. Most of these states are extremely massive but I have proposed that leptons can appear also in color octet partial waves with light masses and there is indeed some evidence for pion like states with mass very near to 2mL for all charged lepton generations decaying to lepton-antilepton pairs and gamma pairs also p-adically scaled up variant having masses coming as octaves of the lowest state is reported for the tau-pion (see this).

Since leptons move in triality zero color partial waves, color does not distinguish between lepton and anti-lepton so that also leptons with the same charge can in principle form a pion-like color singlet with charge +/-2. This is of course not possible for quarks. In the recent case the p-adic prime should be such that the mass for the color octet muon is 105/2 GeV which is about 29m(μ), where m(μ) =105.6 MeV is the mass of muon. Therefore the color octet muons would correspond to p≈2k, k=k(μ)-2× 9=113-18 =95, which not prime but is allowed by the p-adic length scale hypothesis.

But why just k=95? Is it an accident that the scaling factor is same as between the mass scales of the ordinary hadron physics characterized by M107 and M89 hadron physics? If one applies the same argument to tau leptons characterized by M107, one finds that like sign tau pairs should result from pairs of M89 tau leptons having mass m=512×1.776 GeV= 909 GeV. The mass of resonance would be twice this. For electron one has m= 512*.51 MeV= 261.6 MeV with resonance mass equal to 523.2 MeV. Skeptic would argue that this kind of states should have been observed for long time ago if they really exist.

Production of parallel gluon pairs from the decay of strings of M89 hadron physics as source of the leptomesons?

The production mechanism would be via two-gluon intermediate states. Both gluons would decay to unbound colored lepton-antilepton pair such that the two colored leptons and two antileptons would fuse to form two like sign lepton pairs. This process favors gluons moving in parallel. The required presence of also other like sign lepton pair in the state might allow to kill the hypothesis easily.

The presence of parallel gluons could relate to the TGD explanation for the correlated charged particle pairs observed in proton proton collisions (QCD predicts quark gluon plasma and the absence of correlations) in terms of M89 hadron physics (see the earlier posting). The decay of M89 string like objects is expected to produce not only correlated charged pairs but also correlated gluon pairs with members moving in parallel or antiparallel manner. Parallel gluons could produce like sign di-muons and di-electrons and even pairs of like sign μ and e. In the case of ordinary hadron physics this mechanism would not be at work so that one could understand why resonances with electron number two and mass 523 MeV have not been observed earlier.

Even leptons belonging to different generations could in principle form this kind of states and Phil Gibbs has represented a graph which he interprets as providing indications for a state with mass around 105 GeV decaying to like sign μe pairs. In this case one would however expect that mass is roughly 105/2 GeV since electron is considerably lighter than muon in given p-adic length scale.

The decay of bound states of two colored leptons with same (or opposite) charge would require a trilinear coupling gLL8 analogous to magnetic moment coupling. Color octet leptons L8 would transform to ordinary leptons by gluon emission.

To sum up, if the rumor is true M89 hadron physics is beginning to demonstrate its explanatory power. The new hadron physics would explain the correlated charged particle pairs not possible to understand in high energy QCD. The additional gamma pair background resulting from the decays of M89 pions could explain the two-gamma anomaly of Higgs decays, and also the failure to get same mass for the Higgs from ZZ and gamma-gamma decays. One should not forget that M89 pion explains the Fermi bump around 135 GeV. It would also explain the anomalous like sign lepton pairs if one accepts TGD view about color.

For background see the chapter New Particle Physics Predicted by TGD: Part I of "p-Adic Length Scale Hypothesis and Hierarchy of Planck constants".

Friday, December 21, 2012

The recent situation concerning Higgs

Most bloggers have said something about the latest ATLAS results concerning Higgs. I also mentioned this issue in previous posting: because of the importance of Higgs issue I glue below what I said earlier.

Two-gamma anomaly persists but bloggers still want to forget it. Additional anomaly manifesting itself as different estimates for Higgs mass from the observation of decays to gamma pairs and Z pairs has emerged. It is very difficult to believe that there could be two Higgses with very nearly the same mass. The neglect of the existence of some wide resonance (in TGD Universe M89 pion decaying to gamma pairs) producing two-gamma background could lead two-gamma excess and also to problems in mass determination. Phil Gibbs mentions also the digamma excess which ranges up to 200 GeV. Sooner or later one must perhaps take it seriously.

Higgs has been a stone in the toe of TGD. The problem has been the lack of classical space-time correlate for it. No wonder that in the case of Higgs I have developed a large number of alternative scenarios with and without Higgs like particle.

At this moment it seems clear that Higgs like particle exists although it is far from clear whether it has standard model couplings. If TGD has QFT limit and if one believes that Higgs mechanism is the only manner to model the particle massivation in QFT context, then Higgs mechanism would provide a mimicry of p-adic massivation but not its fundamental description. p-Adic thermodynamics is required for a microscopic description. Higgs vacuum expectation could have space-time counterpart at microscopic level and correspond to CP2 part for the trace of the second fundamental form assignable to string world sheet (if string world sheet is minimal surface in space-time as one might expect, it is not minimal surface in imbedding space (meaning vanishing Higgs expectation) except under very special conditions).

The too high decay rate of Higgs like state to gamma pairs is still reported and the mass of Higgs seems to depend slightly on whether it is determined from the production of gamma pairs or Z pairs. This suggests that also something else than Higgs is there. TGD candidate for this something else would be the pion of M89 hadron physics to be discussed below. By a naive scaling estimate for its width as Γ∼ αs M one would obtain width of order 20 GeV.

The identification as the 135 GeV particle for which Fermi telescope finds evidence as M89 pion is rather suggestive. This suggests that the anomalously high rate for the production of gamma pairs could be due to the decays of M89 pion providing an additional background. Due to this background also the determination of the mass of the Higgs like state could lead to different results for gamma pairs and Z pairs in ATLAS.

The rate for the production of gamma pairs is somewhat too high up to cm energy of gamma pair of order 200 GeV. May be this effect could be understood in terms of satellites of M89 pion with mass difference of order 20 GeV. These satellites would be scaled up variants of satellites of ordinary pion(and also other hadrons) for which evidence has been found recently and explained in TGD framework in terms of infared Regge trajectories. Of course, not a single particle physicist in CERN takes this kind of idea seriously since ordinary low energy hadron physics is regarded as a closed chapter of particle physics in higher energy circles.

Both Fermi satellite and LHC have provided interesting data concerming the existence of M89 hadron physics. The standard interpretation for the unexpected correlations for charged particle pairs meaning that they tend move either in parallel or antiparallel manner in heavy ion collisions detected already by RHIC for seven years ago and - even more surprisingly - in proton proton collisions detected by LHC for about two years ago are in terms of color spin glass. In quark gluon plasma one does not expect the correlations. Color spin glass has got support from AdS/CFT correspondence but the model is not fully consistent with the experimental data.

TGD suggests an interpretation in terms of decays of string like objects possible in low energy M89 hadron physics but not in high energy QCD. The 135 GeV particle suggested by Fermi data could be pion of M89 physics rather than dark matter particle.

We must however wait patiently until statistics possibly shows that these effects are real. Until this possibly happens colleagues continue to believe on standard model and direct their efforts to the elimination of new variants of SUSY.

Wednesday, December 19, 2012

Progress during last year in TGD III: consciousness and quantum biology

From the point of view of physicalism biology and neuroscience can be seen as gigantic collections of anomalies and a treasure trove for a theoretician with an open mind. By its inherent fractality TGD predicts new physics in all scales and the new view about quantum jump and predicts mechanisms of macroscopic quantum coherence make the attempts to explain these anomalies irresistible.

TGD inspired theory of consciousness

The key problem of TGD inspired theory of consciousness has been from the beginning the relationship between geometric time and subjective time assigned to the sequence of quantum jumps with quantum jump identified as moment of consciousness. Zero energy ontology poses powerful constraints on the picture and it is now possible to understand how the arrow of geometric time is induced both at the space-time level and the level of imbedding space.

The resulting vision is in conflict with the existing belief system identifying these two times and known to lead to paradoxes. Situation is same as in the case of revolution implied by special relativity: effects like time dilation were highly counter intuitive in the world view which assumed absolute time.

The identification of precise mechanism for what dualist would cal matter mind interaction are also important and the proposed crazy explanation of the reported psychokinetic effects on bits sequences stored in computer memory could apply also to living matter.

The notion of magnetic body

The concept of magnetic body derives from the identification of classical fields in terms of induced gauge potentials and topological field quantization. The hierarchy of Planck constants predicts hierarchy of macrocopically quantum coherent phases assigned with the magnetic bodies. The dynamics of the magnetic body includes phase transitions changing the value of Planck constant and thus inducing change of quantum lengths and reconnections of flux tubes changing the topology of the web formed by the flux tubes. These universal mechanisms allow completely new insights to bio-catalysis, to the ability of biomolecules to find themselves in the dense molecular soup, and on the synchrony of bio-chemical reactions. One obtains also a concrete realization for the idea about living matter as a hologram.

Negentropic entanglement and life in the intersection of matter and mind

The notion of negentropic entanglement encourages the identification of life as something residing in the intersection of realities and p-adicities ("matter and mind"). From TGD viewpoint biology and neurosciences become treasure troves of anomalies with precise data. EEG and its various variants generalize to fractal hierarchies in frequency domain and can be interpreted as a tool for communications between biological and magnetic body. Paranormal phenomena (or whatever word one wants to use) turn out to have an explanation in terms of the mechanisms used by the magnetic body to control biological body and receive sensory input from it.

Metabolism has an interpretation as a manner to transfer or generate negentropic entanglement serving as a quantum correlate of conscious information.

Models for DNA and genetic code

I have done considerable work to develop speculative models about DNA based on the notion of magnetic body. For instance, the model for DNA as a topological quantum computer relies on the assumption that DNA nucleotides and lipids of cell membrane are connected by magnetic flux tubes whose braiding defines the programs of resulting topological quantum computer. This is just a one particular example since flux tube connections would quite generally make living system to behave as a coherent whole and braiding would realized both tqc programs and memory.

Progress during last year in TGD II: theoretical aspects of TGD


In this posting I will summarize the progress made in TGD itself during this year. One category of problems relates to the interpretation of TGD and its relationship to existing theories, to the understanding of the preferred extremals of Kähler action and solutions of the modified Dirac action, to the construction of the generalized Feynman diagrams and to a more precise view about what particles are in this framework. Zero energy ontology is now a basic pillar of TGD and should be understood better. One should also develop the understanding about the fusion of real physics and various p-adic physics inspired by the success of p-adic mass calculations and required by number theoretical universality, about the effective hierarchy of Planck constants predicting dark matter hierarchy, and about hyperfinite factors allowing to realize the notion of finite measurement/cognitive resolution.

The interpretation of TGD

Last years have meant impressive progress in the interpretation of TGD both at classical and quantum level: here one could speak about refinement of the ontology of TGD. These levels are of course related by quantum classical correspondence and this principle has demonstrated its amazing power. The notion of many-sheeted space-time is central.

Basic argument against TGD

Perhaps the strong objection against TGD is that linear superposition for classical fields is lost. The linear superposition is however central starting point of field theories. Many-sheeted space-time allows to circumvent this argument about which I became conscious of just during this year - about 34 year after the discovery of TGD!

The replacement of linear superposition of fields with the superposition of their effecs meaning that sum is replaced with set theoretic union for space-time sheets. This simple observation has far reaching consequences: it becomes possible to replace the dynamics for a multitude of fields with the dynamics of space-time surfaces with only 4 imbedding space coordinates as primary dynamical variables.

Quantum classical correspondence and quantum ergodicity

Quantum classical correspondence has been one of the guiding principles of TGD. The newest conjecture generated by quantum classical correponds is quantum ergodicity. Quantum ergodicity states that quantal correlation functions for classical field like quantities in zero energy state are identical with the classical correlation functions for a any preferred extremal in their superposition. Single preferred extremal represents entire zero energy state so that all space-time surfaces in the quantum superposition of parallel classical worlds are equivalent observationally.

Although zero energy ontology (S-matrix is relaced with M-matrix definign "square root" of density matrix) and 4-D spin glass degeneracy suggest that this principle is satisfied only by the outcomes of state function reduction, it is extremely powerful if it really works.

The effective hierarchy of Planck constants and dark matter

In TGD framework dark matter could be understand as phases of matter with scaled up value of effective Planck constant. This explanation distinguishes sharply between TGD and competitors and leads to a completely new view about quantum biology based on the notion of magnetic body carrying dark matter. TGD leads also to a view about dark energy as Kähler magnetic energy.

The theoretical understanding of the effective hierarchy of Planck constants in terms of space-time topology has developed during this idea. The newest idea is that the effective n-sheeted cover of imbedding space to which effective value of Planck constant hbareff=nhbar is assigned corresponds to an n-furcation natural in the non-linear dynamics of Kähler action by its enormous vacuum degeneracy. The list about the applications to living matter has been steadily growing.

Strong form of general coordinate invariance and holography

Strong form of general coordinate invariance (GCI) implies strong form of holography. The outcome is TGD counterpart of AdS/CFT correspondence. Bulk is replaced with space-time surface and strings with 2-D string world sheets carrying fermionic fields (right handed neutrino is exception and is delocalized into entire space-time surface). Partonic 2-surfaces at the boundaries of CDs and the 4-D tangent space data at them would code for the quantum dynamics. Interior dynamics would provide classical correlates for quantum states - say classical correlation functions identical to their quantum counterparts if quantum ergodicity holds true.

One outcome is a new view about black holes replacing the interior of blackhole with a space-time region of Euclidian signature of induced metric and identifiable as analogs of lines of generalized Feynman diagrams. In fact, black hole interiors are only special cases of Eucdlian regions which can be assigned to any physical system. This means that the description of condensed matter as AdS blackholes is replaced in TGD framework with description using Euclidian regions of space-time.

Zero energy ontology

Zero energy ontology (ZEO) has inspired detailed development of the views about the relationship between geometric and subjective time and led to highly non-trivial picture challenging the existing beliefs. No final conclusions are possible yet but I believe that the understanding continues to grow. ZEO has led also to a highly detailed view about generalized Feynman diagrammatics.

p-Adic physics

p-Adic physics, p-adic mass calculations, p-adic length scale hypothesis and the integration of various p-adic physics and real physics to a bigger whole have continued to be sources of challenges and inspiration. In biological and neuroscience applications number theoretic entropy identifiable as negentropy has led to a vision about living matter as something residing in the intersection of real and p-adic physics.

Hyperfinite factors

The mathematics of hyperfinite factors is too difficult for an theoretical physicist like me but still considerable progress has taken place. All new visions generate a great burst of ideas and so did also hyperfinite factors as I realized their importance for about seven years ago. The subsequent progress has been mostly selection of the fittest ones with internal consistency defining the most powerful evolutionary pressure. During this year emerged a Fresh view about hyperfinite factors.

Twistors and TGD

Twistors are the hot topic of recent day theoretical physics. ZEO allows to make conjectures about connections with the twistor approach. I do not have the needed technical competence so that I can only try to see the situation at the level of principles.

The basic physical idea of generalized Feynman diagrammatics is that the fermions propagating along the lines of generalized Feynman diagrams (associated with braids at light-like 3-surfaces at which the signature of the induced metric changes) are massless. The condition that also virtual fermions are massless leads to a non-trivial diagrammatics if the sign of the energy can have both values for the virtual wormhole throats. The condition is extremely powerful and eliminates most diagrams and also both IR and UV divergences and allows to understand how the massivation of external particle can be consistent with conformal invariance.

Masslessness is the basic condition making possible to express kinematics in terms of twistors. What one expects is that after functional integration the resulting amplitudes satisfy the Yangian symmetry characterizing also twistor diagrams and fixing them to a high degree. Also Yangian symmetry has a natural generalization in TGD framework.

Preferred extremals and solutions of the modified Dirac equation

The last years have meant rapid progress in the understanding of TGD at the fundamental level. The key concept of TGD is the notion of preferred extremal. It roughly means that one can assign to a collection of 3-surfaces at the ends of a causal diamond (CD) a unique space-time surface. A realization of holography would be in question.

Strong form of GCI leads to the strong form of holography stating that light-like 3-surfaces connecting the ends of CD and space-like 3-surfaces the ends of CD are equivalent choices. Therefore partonic 2-surface defined as their intersections plus 4-D tangent space data at them would fix the quantum physics in ZEO.

One can of course wonder whether the space-like 3-surfaces and light-like 3-surfaces are completely unique from the preferred extremal property or whether they are unique apart from conformal transformations assignable to the light-like coordinate of light-like 3-surface or to the light-like coordinate of δ CD× CP2. This interpretation would conform with the interpretation of these conformal transformations as gauge transformations. These transformations would extend to ordinary conformal transformations at string world sheets (with Minkowskian signature and hypercomplex structure), which are carriers of spinor fields in the proposed general solution of the modified Dirac equation based on the requirement of the conservation of electric charge.

But what are these preferred extremals? This is the key question. The first guess was that they are absolute minima of Kähler action. This option did not resonate with the number theoretic visions for the simple reason that minimization for p-adic valued functions does not make sense. I have gradually gained rather detailed knowledge about propertie of preferred extremals. For instance, the reduction of the Kähler action to Chern-Simons terms coming from Minkowskian and Euclidian regions (and differing by imaginary unit) gives a partial realization of the holography and boils down to the vanishing of jKμAμ, where jK denotes Kähler current.

What I regard as a breakthrough came during this year and reduces the construction of preferred extremals to a generalization of the notion of complex structure. In Minkowskian regions of space-time surface I call this structure Hamilton-Jacobi structure identifiable as a composite of complex structure and hyper-complex structure. In Hamilton-Jacob coordinates the field equations reduce to conditions on 4-metric completely analogous to the condition gzz=0 for Euclidian string world sheets.

The field equations are equivalent to minimal surface equations although action is of course something different from 4-volume which is definitely an unphysical choice. As a consequence, induced gamma matrices satisfy the consistency condition DμΓμ=0 giving additional supercharges besides those associated with modified gamma matrices.

Also Einstein equations with cosmological term follow as a consistency condition requiring that the Maxwell energy momentum tensor has vanishing divergence. Newton's constant and cosmological constant are predictions rather than inputs as in the standard theory. Given space-time sheet has constant value of Ricci scalar which has far reaching consequences.

I already mentioned that also a beautiful solution ansatz for the modified Dirac equations emerges from the conservation of electric charged defined in spinorial sense. All modes of the induced spinor field except right-handed neutrino are localized on 2-D string world sheets. This implies automatically braid picture: the boundaries of the string world sheets at light-like and space-like 3-surfaces are 1-D curves identifiable as light-like and space-like braids strands. This also conforms with the vision that discretization at partonic 2-surfaces identifiable as a space-time correlate of finite measurement resolution follows from the dynamics automatically so that the dynamics is highly self-referential.

The improved understanding of the modified Dirac action leads also to a detailed microscopic view about elementary particle as closed string like objects. Knotting is one topological phenomenon possible because of the dimension of space-time surface. This picture has concrete implications for the model of the observed elementary particles.

Mathematical ideas inspired by TGD

I do not regard myself as a mathematician in the technical sense of the word. TGD has however forced to generalize existing mathematical concepts, and to even formulate new mathematical notions besides the use of existing mathematics still relatively new for theoretical physicists.

Classical TGD relies on existing mathematical concepts and the main challenges are the understanding of preferred extremals and solutions of the modified Dirac equation. There are several independent conjectures about preferred extremals which should be proven to be right or wrong.

Quantum TGD provides challenging examples of yet non-existing mathematics such as the generalization of loop space geometry to that of WCW and construction of WCW spinor structure. Infinite-dimensional isometry group fixes these structures more or less uniquely but there is huge amount of work to do. The theory hyper-finite factors seems to require an approach generalizing the existing thermodynamical approach to TGD framework which can be seen as a "square root" of thermodynamics. Number theoretical universality requires the fusion of p-adic and real number fields to a larger structure and there are several challenges involved (say precise definition of the notion of integral in p-adic context) attacked also by the leading mathematicians of our time. Infinite primes is a TGD inspired notion having an interpretation as a repeated second quantization of a super-symmetric arithmetic quantum field theory with states labelled by primes and their generalization to infinite primes. There are strong indications that this hierarchy relates directly to various hierarchies of quantum TGD.

During this year a burst of really crazy ideas was inspired by TGD, and I still feel myself rather uneasy with this stuff. Certainly it takes years to find the surviving ideas if any. The key idea is roughly that the standard arithmetics with its sum and product generalize to an arithmetics of Hilbert spaces with sum replaced with direct sum and product with tensor product. This suggests a calculus of Hilbert spaces: one can define Hilbert spaces with dimension which can be also negative integer, rational, algebraic, or even transcendental, one can define Taylor series of Hilbert spaces. By mapping Hilbert space to a single number defined by its dimension one would obtain the ordinary calculus. Everything that can be done with ordinary numbers could be done with Hilbert spaces. This construction can be repeated just like the construction of infinite primes. One can replace the points of Hilbert space with Hilbert spaces and so on... This of course goes completely over the human head.

The question is whether this crazy construction might have some sensible physical interpretation. What made me to take this crazy idea half-seriously was that for generalized Feynman diagrams there are two basic vertices: the generalization of the 3-vertex of ordinary Feynman diagrams having interpretation as tensor product and the generalization of stringy 3-vertex having very natural interpretation in terms of direct sum (in string models the interpretation is in terms of tensor product).

Progress during last year in TGD I: Particle physics

In this and subsequent postings I try to present an overview about the basic themes that have motivated blog articles during this year with links to the appropriate postings. This also helps me to get a bird's eye of view to what I have been doing during the year;-).

In these postings I will consider first the experimental side, then theoretical aspects of TGD, and finally quantum biology and TGD inspired theory of consciousness.

One can say that on the experimental side the year has been dominated by Higgs, SUSY, and dark matter. On the theoretical side the developments related to the understanding of the preferred extremals of Kähler action and of solutions of the modified Dirac action have dominated the scene but also other important ideas and insights have emerged. In quantum biology new applications for the notions of magnetic body and negentropic entanglement have emerged. In TGD inspired theory of consciousness zero energy ontology (ZEO) has led to a more detailed view about the relationship between geometric time and experienced time leading to highly non-trivial modification of existing manners of thinking.

The media-hot issues have been mostly in particle physics sector. The buzz words have been Higgs, SUSY, and dark matter. Scaled up variante of hadron physics is one of the most important TGD predictions but represents something totally new for the mainstream and blogger community. The results from LHC and Fermi satellite have been especially interesting in this respect.

1. Higgs issue

Higgs has been a stone in the toe of TGD. The problem has been the lack of classical space-time correlate for it.
No wonder that in the case of Higgs I have developed a large number of alternative scenarios with and without Higgs like particle.

At this moment it seems clear that Higgs like particle exists although it is far from clear whether it has standard model couplings. If TGD has QFT limit and if one believes that Higgs mechanism is the only manner to model the particle massivation in QFT context, then Higgs mechanism would provide a mimicry of p-adic massivation but not its fundamental description. p-Adic thermodynamics is required for a microscopic description. Higgs vacuum expectation could have space-time counterpart at microscopic level and correspond to CP2 part for the trace of the second fundamental form assignable to string world sheet (if string world sheet is minimal surface in space-time as one might expect, it is not minimal surface in imbedding space (meaning vanishing Higgs expectation) except under very special conditions).

The too high decay rate of Higgs like state to gamma pairs is still reported and the mass of Higgs seems to depend slightly on whether it is determined from the production of gamma pairs or Z pairs. This suggests that also something else than Higgs is there. TGD candidate for this something else would be the pion of M89 hadron physics to be discussed below. By a naive scaling estimate for its width as Γ∼ αs M one would obtain width of order 20 GeV.

The identification as the 135 GeV particle for which Fermi telescope finds evidence as M89 pion is rather suggestive. This suggests that the anomalously high rate for the production of gamma pairs could be due to the decays of M89 pion providing an additional background. Due to this background also the determination of the mass of the Higgs like state could lead to different results for gamma pairs and Z pairs in ATLAS.

The rate for the production of gamma pairs is somewhat too high up to cm energy of gamma pair of order 200 GeV. May be this effect could be understood in terms of satellites of M89 pion with mass difference of order 20 GeV. These satellites would be scaled up variants of satellites of ordinary pion(and also other hadrons) for which evidence has been found recently and explained in TGD framework in terms of infared Regge trajectories. Of course, not a single particle physicist in CERN takes this kind of idea seriously since ordinary low energy hadron physics is regarded as a closed chapter of particle physics in higher energy circles.

2. M89 hadron physics

M89 hadron physics is one of the key "almost"-predictions of TGD at LHC. Both Fermi satellite and LHC have provided interesting data in this respect. The standard interpretation for the unexpected correlations for charged particle pairs meaning that they tend move either in parallel or antiparallel manner in heavy ion collisions detected already by RHIC for seven years ago and - even more surprisingly - in proton proton collisions detected by LHC for about two years ago are in terms of color spin glass. In quark gluon plasma one does not expect the correlations. Color spin glass has got support from AdS/CFT correspondence but the model is not fully consistent with the experimental data.

TGD suggests an interpretation in terms of decays of string like objects possible in low energy M89 hadron physics but not in high energy QCD. The 135 GeV particle suggested by Fermi data could be pion of M89 physics rather than dark matter particle.

3. New hadron physics suggested by TGD

TGD view about strong interactions differs in many respects from that provided by QCD. In particular, the interpretation of color quantum numbers is not as spin like quantum numbers but in terms of partial waves in CP2 degrees of freedom. The many-sheeted space-time also leads to a view about both partons and hadrons as 3-D surfaces and the notion of color magnetic body is expected to be central in the description of hadrons at low energies.

There exists recent evidence for satellites of ordinary hadrons with mass differences having the scale of 20-40 MeV. TGD suggest an explanation in terms of new physics assignable to IR color magnetic flux tubes. This physics should make itself visible also in M89 physics via satellites of M89 hadrons, in particular pion whose decays would provide additional gamma pair background perhaps relating to the too high decay rate of Higgs like state to gamma pairs.

4. N=1 SUSY

LHC has reported very strong bounds on the parameters of the models based on N=1 SUSY and the models are getting increasinly complicated. This is also a bad news for super string models. In fact, the Russian discoverer of the supersymmetry believes that something is badly wrong with the standard SUSY, and one should try something more imaginative rather than tinkering with models which do not work. He even talks about a lost generation of theoretical physicists. I can only agree.

N =1 SUSY and thus standard SUSY is excluded in TGD framework from the beginning by the dimension 8 of the imbedding space. For long time I however thought that covariantly constant right-handed neutrino could produce it approximately. It seems now that this is not the case although one has different kind of badly broken large N SUSY. The core of argument is that since covariantly constant right handed neutrino decouples from all interactions (even gravitational!), its behavior cannot combine with particle to form sparticle as strongly spin-correlated pair so that right-handed neutrinos behave as their own phase.

5. Dark matter

Dark matter is one of the hot topics of the recent day physics. TGD view about various forms of dark matter differs dramatically from the standard views and means different interpretation for the observations interpreted as indications for the existence of dark matter. The hierarchy of phases of matter characterized by an effective value of Planck constant coming as a multiple of Planck constant would behave like dark matter as far as vertices of Feynman diagrams are considered.

Galactic dark matter could be identified as Kähler magnetic energy of magnetic flux tubes originated from primordial cosmic strings. One can assign to these objects a gigantic value of an effective Planck constant as "gravitational Planck constant". The magnetic energy has an identification as dark energy in TGD framework. Distant stars in the galactic plane are predicted to have contant velocity spectrum without any further assumptions. The motion of astrophysical objects would be however free along the cosmic string containing galaxies around it like pearls in necklace.

During the last year Fermi satellite has produced valuable data consistent with TGD view.

6. Miscellaneous

There are also other new physics topics related to physics that I have written about.


Monday, December 10, 2012

Is there a connection between preferred extremals and AdS4/CFT correspondence?

The preferred extremals satisfy Einstein Maxwell equations with a cosmological constant and have negative curvature for negative value of Λ. 4-D space-times with hyperbolic metric provide canonical representation for a large class of four-manifolds and an interesting question is whether these spaces are obtained as preferred extremals and/or vacuum extremals.

4-D hyperbolic space with Minkowski signature is locally isometric with AdS4. This suggests a connection with AdS4/CFT correspondence of M-theory. The boundary of AdS would be now replaced with 3-D light-like orbit of partonic 2-surface at which the signature of the induced metric changes. The metric 2-dimensionality of the light-like surface makes possible generalization of 2-D conformal invariance with the light-like coordinate taking the role of complex coordinate at light-like boundary. AdS would presumably represent a special case of a more general family of space-time surfaces with constant Ricci scalar satisfying Einstein-Maxwell equations and generalizing the AdS4/CFT correspondence.


For the ordinary AdS5 correspondence empty M4 is identified as boundary. In the recent case the boundary of AdS4 is replaced with a 3-D light-like orbit of partonic 2-surface at which the signature of the induced metric changes. String world sheets have boundaries along light-like 3-surfaces and space-like 3-surfaces at the light-like boundaries of CD. The metric 2-dimensionality of the light-like surface makes possible generalization of 2-D conformal invariance with the light-like coordinate taking the role of hyper- complex coordinate at light-like 3-surface. AdS5× S5 of M-theory context is replaced by a 4-surface of constant Ricci scalar in 8-D imbedding space M4× CP2 satisfying Einstein-Maxwell equations. A generalization of AdS4/CFT correspondence would be in question. Note however that the accelerated expansion of the Universe requires positive value of Λ and favors De Sitter Space dS4 instead of AdS4.

These observations give motivations for finding whether AdS4 or dS4 or both allow an imbedding as vacuum extremal to M4× S2⊂ M4× CP2, where S2 is a homologically trivial geodesic sphere of CP2. It is easy to guess the general form of the imbedding by writing the line elements of, M4, S2, and AdS4.

  1. The line element of M4 in spherical Minkowski coordinates (m,rM,θ,φ) reads as

    ds2= dm2-drM2-rM2dΩ2 .

  2. Also the line element of S2 is familiar:

    ds2=- R2(dΘ2+sin2(θ)dΦ2) .

  3. By visiting in Wikipedia one learns that in spherical coordinate the line element of AdS4 is given by

    ds2= A(r)dt2-(1/A(r))dr2-r2dΩ2 ,

    A(r)= 1+y2 , y = r/r0 .

  4. From these formulas it is easy to see that the ansatz is of the same general form as for the imbedding of Schwartschild-Nordstöm metric:

    m= Λ t+ h(y) , rM= r ,
    Θ = s(y) , Φ= ω× (t+f(y)) .

    The non-trivial conditions on the components of the induced metric are given by

    gtt= Λ2-x2sin2(Θ) = A(r) ,

    gtr= 1/r0[Λ dh/dy -x2sin2(θ) df/dr]=0 ,

    grr= 1/r02[(dh/dy)2 -1- x2sin2(θ)(df/dy)2- R2(dΘ/dy)2]= -1/A(r) ,

    x=Rω .

By some simple algebraic manipulations one can derive expressions for sin(Θ), df/dr and dh/dr.
  1. For Θ(r) the equation for gtt gives the expression

    sin2(Θ)= P/x2 ,

    P= Λ2 -A =Λ2-1-y2 .

    The condition 0≤ sin2(Θ)≤ 1 gives the conditions

    (Λ2-x2-1)1/2 ≤ y≤ (Λ2-1)1/2 .

    Clearly only a spherical shell is possible.

  2. From the vanishing of gtr one obtains

    dh/dy = ( P/Λ)× df/dy ,


  3. The condition for grr gives

    (df/dy)2 =[r02/AP]× [A-1-R2(dΘ/dy)2] .

    Clearly, the right-hand side is positive if P≥ 0 holds true and RdΘ/dy is small.
    From this condition one can solved by expressing dΘ/dy using chain rule as

    (dΘ/dy)2=x2y2/[P (P-x2)] .

    One obtains

    (df/dy)2 = [Λ r02y2/AP]× [(1+y2)-1 -x2(R/r0)2 [P(P-x2)]-1)] .

    The right hand side of this equation is non-negative for certain range of parameters and variable y.
    Note that for r0>> R the second term on the right hand side can be neglected. In this case it is easy to integrate f(y).

The conclusion is that AdS4 allows a local imbedding as a vacuum extremal. Whether also an imbedding as a non-vacuum preferred extremal to homologically non-trivial geodesic sphere is possible, is an interesting question. The only modification in the case of De Sitter space dS4 is the replacement of the function A= 1+y2 appearing in the metric of AdS4 with A=1-y2. Also now the imbedded portion of the metric is a spherical shell. This brings in mind TGD inspired model for the final state of the star which is also a spherical shell. p-Adic length scale hypothesis motivates the conjecture that stars indeed have onion-like layered structure consisting of shells, whose radii are consistent with p-adic length scale hypothesis. This brings in mind also Titius-Bode law.

For details and background see the chapter The recent vision about preferred extremals and solutions of the modified Dirac equation of "Physics as Infinite-dimensional Geometry", or the article with the title "Do geometric invariants of preferred extremals define topological invariants of space-time surface and code for quantum physics?".

Sunday, December 09, 2012

How coupling constant evolution could make itself visible as properties of preferred extremals?


Quantum classical correspondence states that all aspects of quantum states should have correlates in the geometry of preferred extremals. In particular, various elementary particle propagators should have a representation as properties of preferred extremals. This would allow to realize the old dream about being able to say something interesting about coupling constant evolution although it is not yet possible to calculate the M-matrices and U-matrix. Hitherto everything that has been said about coupling constant evolution has been rather speculative arguments except for the general vision that it reduces to a discrete evolution defined by p-adic length scales. General first principle definitions are much more valuable than ad hoc guesses even if the latter give rise to explicit formulas.

In quantum TGD and also at its QFT limit various correlation functions in given quantum state code for its properties. These correlation functions should have counterparts in the geometry of preferred extremals. Even more: these classical counterparts for a given preferred extremal ought to be identical with the quantum correlation functions for the superposition of preferred extremals.

  1. The marvelous implication of quantum ergodicity would be that one could calculate everything solely classically using the classical intuition - the only intuition that we have. Quantum ergodicity would also solve the paradox raised by the quantum classical correspondence for momentum eigenstates. Any preferred extremal in their superposition defining momentum eigenstate should code for the momentum characterizing the superposition itself. This is indeed possible if every extremal in the superposition codes the momentum to the properties of classical correlation functions which are identical for all of them.

  2. The only manner to possibly achieve quantum ergodicity is in terms of the statistical properties of the preferred extremals. It should be possible to generalize the ergodic theorem stating that the properties of statistical ensemble are represented by single space-time evolution in the ensemble of time evolutions. Quantum superposition of classical worlds would effectively reduce to single classical world as far as classical correlation functions are considered. The notion of finite measurement resolution suggests that one must state this more precisely by adding that classical correlation functions are calculated in a given UV and IR resolutions meaning UV cutoff defined by the smallest CD and IR cutoff defined by the largest CD present.

  3. The skeptic inside me immediately argues that TGD Universe is 4-D spin glass so that this quantum ergodic theorem must be broken. In the case of the ordinary spin classes one has not only statistical average for a fixed Hamiltonian but a statistical average over Hamiltonians. There is a probability distribution over the coupling parameters appearing in the Hamiltonian. Maybe the quantum counterpart of this is needed to predict the physically measurable correlation functions.

    Could this average be an ordinary classical statistical average over quantum states with different classical correlation functions? This kind of average is indeed taken in density matrix formalism. Or could it be that the square root of thermodynamics defined by ZEO actually gives automatically rise to this average? The eigenvalues of the "hermitian square root " of the density matrix would code for components of the state characterized by different classical correlation functions. One could assign these contributions to different "phases".

  4. Quantum classical correspondence in statistical sense would be very much like holography (now individual classical state represents the entire quantum state). Quantum ergodicity would pose a rather strong constraint on quantum states. This symmetry principle could actually fix the spectrum of zero energy states to a high degree and fix therefore the M-matrices given by the product of hermitian square root of density matrix and unitary S-matrix and unitary U-matrix having M-matrices as its orthonormal rows.

  5. In TGD inspired theory of consciousness the counterpart of quantum ergodicity is the postulate that the space-time geometry provides a symbolic representation for the quantum states and also for the contents of consciousness assignable to quantum jumps between quantum states. Quantum ergodicity would realize this strongly self-referential looking condition. The positive and negative energy parts of zero energy state would be analogous to the initial and final states of quantum jump and the classical correlation functions would code for the contents of consciousness like written formulas code for the thoughts of mathematician and provide a sensory feedback.

How classical correlation functions should be defined?
  1. General Coordinate Invariance and Lorentz invariance are the basic constraints on the definition. These are achieved for the space-time regions with Minkowskian signature and 4-D M4 projection if linear Minkowski coordinates are used. This is equivalent with the contraction of the indices of tensor fields with the space-time projections of M4 Killing vector fields representing translations. Accepting ths generalization, there is no need to restrict oneself to 4-D M4 projection and one can also consider also Euclidian regions identifiable as lines of generalized Feynman diagrams.

    Quantum ergodicity very probably however forces to restrict the consideration to Minkowskian and Euclidian space-time regions and various phases associated with them. Also CP2 Killing vector fields can be projected to space-time surface and give a representation for classical gluon fields. These in turn can be contracted with M4 Killing vectors giving rise to gluon fields as analogs of graviton fields but with second polarization index replaced with color index.

  2. The standard definition for the correlation functions associated with classical time evolution is the appropriate starting point. The correlation function GXY(τ) for two dynamical variables X(t) and Y(t) is defined as the average GXY(τ)=∫T X(t)Y(t+τ)dt/T over an interval of length T, and one can also consider the limit T→ ∞. In the recent case one would replace kenotau with the difference m1-m2=m of M4 coordinates of two points at the preferred extremal and integrate over the points of the extremal to get the average. The finite time interval T is replaced with the volume of causal diamond in a given length scale. Zero energy state with given quantum numbers for positive and negative energy parts of the state defines the initial and final states between which the fields appearing in the correlation functions are defined.

  3. What correlation functions should be considered? Certainly one could calculate correlation functions for the induced spinor connection given electro-weak propagators and correlation functions for CP2 Killing vector fields giving correlation functions for gluon fields using the description in terms of Killing vector fields. If one can uniquely separate from the Fourier transform uniquely a term of form Z/(p2-m2) by its momentum dependence, the coefficient Z can be identified as coupling constant squared for the corresponding gauge potential component and one can in principle deduce coupling constant evolution purely classically. One can imagine of calculating spinorial propagators for string world sheets in the same manner. Note that also the dependence on color quantum numbers would be present so that in principle all that is needed could be calculated for a single preferred extremal without the need to construct QFT limit and to introduce color quantum numbers of fermions as spin like quantum numbers (color quantum numbers corresponds to CP2 partial wave for the tip of the CD assigned with the particle).

  4. What about Higgs like field? TGD in principle allows scalar and pseudo-scalars which could be called Higgs like states. These states are however not necessary for particle massivation although they can represent particle massivation and must do so if one assumes that QFT limit exist. p-Adic thermodynamics however describes particle massivation microscopically.

    The problem is that Higgs like field does not seem to have any obvious space-time correlate. The trace of the second fundamental form is the obvious candidate but vanishes for preferred extremals which are both minimal surfaces and solutions of Einstein Maxwell equations with cosmological constant. If the string world sheets at which all spinor components except right handed neutrino are localized for the general solution ansatz of the modified Dirac equation, the corresponding second fundamental form at the level of imbedding space defines a candidate for classical Higgs field. A natural expectation is that string world sheets are minimal surfaces of space-time surface. In general they are however not minimal surfaces of the imbedding space so that one might achieve a microscopic definition of classical Higgs field and its vacuum expectation value as an average of one point correlation function over the string world sheet.

For details and background see the chapter The recent vision about preferred extremals and solutions of the modified Dirac equation, or the article with the title "Do geometric invariants of preferred extremals define topological invariants of space-time surface and code for quantum physics?".

Tuesday, December 04, 2012

Preferred extremals of Kähler action as constant curvature manifolds whose geometric invariants are topological invariants



The recent progress in the understanding of the preferred extremals led to a reduction of the field equations to conditions stating for Euclidian signature the existence of Kähler metric. The resulting conditions are a direct generalization of corresponding conditions emerging for the string world sheet and stating that the 2-metric has only non-diagonal components in complex/hypercomplex coordinates. Also energy momentum of Kähler action and has this characteristic (1,1) tensor structure. In Minkowskian signature one obtains the analog of 4-D complex structure combining hyper-complex structure and 2-D complex structure.

The construction lead also to the understanding of how Einstein's equations with cosmological term follow as a consistency condition guaranteeing that the covariant divergence of the Maxwell's energy momentum tensor assignable to Kähler action vanishes. This gives T= kG+Λ g. By taking trace a further condition follows from the vanishing trace of T:

R = 4Λ/k .

That any preferred extremal should have a constant Ricci scalar proportional to cosmological constant is very strong prediction. Note however that both Λ and k∝ 1/G are both parameters characterizing one particular preferred extremal. One could of course argue that the dynamics allowing only constant curvature space-times is too simple. The point is however that particle can topologically condense on several space-time sheets meaning effective superposition of various classical fields defined by induced metric and spinor connection.

The following considerations demonstrate that preferred extremals can be seen as canonical representatives for the constant curvature manifolds playing central role inThurston's geometrization theorem known also as hyperbolization theorem implying that geometric invariants of space-time surfaces transform to topological invariants.

The generalization of the notion of Ricci flow to Maxwell flow in the space of metrics and further to Kähler flow for preferred extremals in turn gives a rather detailed vision about how preferred extremals organize to one-parameter orbits. It is quite possible that Kähler flow is actually discrete. The natural interpretation is in terms of dissipation and self organization.

A. The geometrical invariants of space-time surfaces as topological invariants

An old conjecture inspired by the preferred extremal property is that the geometric invariants of the space-time surface serve as topological invariants. The reduction ofKähler action to 3-D Chern-Simons terms gives support for this conjecture as a classical counterpart for the view about TGD as almost topological QFT. The following arguments give a more precise content to this conjecture in terms of existing mathematics.

  1. It is not possible to represent the scaling of the induced metric as a deformation of the space-time surface preserving the preferred extremal property since the scale of CP2 breaks scale invariance. Therefore the curvature scalar cannot be chosen to be equal to one numerically. Therefore also the parameter R=4Λ/k and also Λ and k separately characterize the equivalence class of preferred extremals as is also physically clear.

    Also the volume of the space-time sheet closed inside causal diamond CD remains constant along the orbits of the flow and thus characterizes the space-time surface. Λ and even k∝ 1/G can indeed depend on space-time sheet and p-adic length scale hypothesis suggests a discrete spectrum for Λ/k expressible in terms of p-adic length scales: Λ/k ∝ 1/Lp2 with p≈ 2k favored by p-adic length scale hypothesis. During cosmic evolution the p-adic length scale would increase gradually. This would resolve the problem posed by cosmological constant in GRT based theories.

  2. One could also see the preferred extremals as 4-D counterparts of constant curvature 3-manifolds in the topology of 3-manifolds. An interesting possibility raised by the observed negative value of Λ is that most 4-surfaces are constant negative curvature 4-manifolds. By a general theorem coset spaces H4/Γ, where H4= SO(1,4)/SO(4) is hyperboloid of M5 and Γ a torsion free discrete subgroup of SO(1,4). Geometric invariants are therefore topological invariants. It is not clear to me, whether the constant value of Ricci scalar implies constant sectional curvatures and therefore hyperbolic space property. It could happen that the space of spaces with constant Ricci curvature contain a hyperbolic manifold as an especially symmetric representative. In any case, the geometric invariants of hyperbolic metric are topological invariants.

    By Mostow rigidity theorem finite-volume hyperbolic manifold is unique for D>2 and determined by the fundamental group of the manifold. Since the orbits under the Kähler flow preserve the curvature scalar the manifolds at the orbit must represent different imbeddings of one and hyperbolic 4-manifold. In 2-D case the moduli space for hyperbolic metric for a given genus g>0 is defined by Teichmueller parameters and has dimension 6(g-1). Obviously the exceptional character of D=2 case relates to conformal invariance. Note that the moduli space in question plays a key role in p-adic mass calculations \cite{allb}{elvafu}.

    In the recent case Mostow rigidity theorem could hold true for the Euclidian regions and maybe generalize also to Minkowskian regions. If so then both "topological" and "geometro" in "Topological GeometroDynamics" would be fully justified. The fact that geometric invariants become topological invariants also conforms with "TGD as almost topological QFT" and allows the notion of scale to find its place in topology. Also the dream about exact solvability of the theory would be realized in rather convincing manner.

These conjectures are the main result of this posting independent of whether the generalization of the Ricci flow discussed in the sequel exists as a continuous flow or possibly discrete sequence of iterates in the space of preferred extremals of Kähler action. My sincere hope is that the reader could grasp how far reaching these result really are.

B. Generalizing Ricci flow to Maxwell flow for 4-geometries and K\"ahler flow for space-time surfaces

The notion of Ricci flow has played a key part in the geometrization of topological invariants of Riemann manifolds. I certainly did not have this in mind when I choose to call my unification attempt "Topological Geometrodynamics" but this title strongly suggests that a suitable generalization of Ricci flow could play a key role in the understanding of also TGD.

B.1. Ricci flow and Maxwell flow for 4-geometries

The observation about constancy of 4-D curvature scalar for preferred extremals inspires a generalization of the well-known volume preserving Ricci flow introduced by Richard Hamilton and defined in the space of Riemann metrics as

dgαβ/dt= -2Rαβ+ (2/D)Ravggαβ .

Here Ravg denotes the average of the scalar curvature, and D is the dimension of the Riemann manifold. The flow is volume preserving in average sense as one easily checks (<gαβdgαβ/dt> =0). The volume preserving property of this flow allows to intuitively understand that the volume of a 3-manifold in the asymptotic metric defined by the Ricci flow is topological invariant. The fixed points of the flow serve as canonical representatives for the topological equivalence classes of 3-manifolds. These 3-manifolds (for instance hyperbolic 3-manifolds with constant sectional curvatures) are highly symmetric. This is easy to understand since the flow is dissipative and destroys all details from the metric.

What happens in the recent case? The first thing to do is to consider what might be called Maxwell flow in the space of all 4-D Riemann manifolds allowing Maxwell field.

  1. First of all, the vanishing of the trace of Maxwell's energy momentum tensor codes for the volume preserving character of the flow defined as

    dgαβ/dt= Tαβ .

    Taking covariant divergence on both sides and assuming that d/dt and Dα commute, one obtains that Tαβ is divergenceless.

    This is true if one assumes Einstein Maxwell equations with cosmological term. This gives

    dgαβ/dt= kGαβ+ Λ gαβ =k Rαβ + (-kR/2+Λ)gαβ .

    The trace of this equation gives that the curvature scalar is constant. Note that the value of the Kähler coupling strength plays a highly non-trivial role in these equations and it is quite possible that solutions exist only for some critical values of αK. Quantum criticality should fix the allow value triplets (G,Λ,αK) apart from overall scaling

    (G,Λ,αK)→ (xG,Λ/x, xαK) .

    Fixing the value of G fixes the values remaining parameters at critical points. The rescaling of the parameter t induces a scaling by x.

  2. By taking trace one obtains the already mentioned condition fixing the curvature to be constant,
    and one can write

    dgαβ/dt= kRαβ -Λ gαβ .

    Note that in the recent case Ravg=R holds true since curvature scalar is constant. The fixed points of the flow would be Einstein manifolds satisfying

    Rαβ= (Λ/k) gαβ .


  3. It is by no means obvious that continuous flow is possible. The condition that Einstein-Maxwell equations are satisfied might pick up from a completely general Maxwell flow a discrete subset as solutions of Einstein-Maxwell equations with a cosmological term. If so, one could assign to this subset a sequence of values tn of the flow parameter t.

  4. I do not know whether 3-dimensionality is somehow absolutely essential for getting the classification of closed 3-manifolds using Ricci flow. This ignorance allows me to pose some innocent questions. Could one have a canonical representation of 4-geometries as spaces with constant Ricci scalar? Could one select one particular Einstein space in the class four-metrics and could the ratio Λ/k represent topological invariant if one normalizes metric or curvature scalar suitably. In the 3-dimensional case curvature scalar is normalized to unity. In the recent case this normalization would give k= 4Λ in turn giving Rαβ= gαβ/4. Does this mean that there is only single fixed point in local sense, analogous to black hole toward which all geometries are driven by the Maxwell flow? Does this imply that only the 4-volume of the original space would serve as a topological invariant?

B.2. Maxwell flow for space-time surfaces

One can consider Maxwell flow for space-time surfaces too. In this case Kähler flow would be the appropriate term and provides families of preferred extremals. Since space-time surfaces inside CD are the basic physical objects are in TGD framework, a possible interpretation of these families would be as flows describing physical dissipation as a four-dimensional phenomenon polishing details from the space-time surface interpreted as an analog of Bohr orbit.

  1. The flow is now induced by a vector field jk(x,t) of the space-time surface having values in the tangent bundle of imbedding space M4× CP2. In the most general case one has Kähler flow without the Einstein equations. This flow would be defined in the space of all space-time surfaces or possibly in the space of all extremals. The flow equations reduce to

    hkl Dα jk(x,t) Dβhl= (1/2)Tαβ .

    The left hand side is the projection of the covariant gradient Dαjk(x,t) of the flow vector field jk(x,t) to the tangent space of the space-time surface. D α is covariant derivative taking into account that jk is imbedding space vector field. For a fixed point space-time surface this projection must vanish assuming that this space-time surface reachable. A good guess for the asymptotia is that the divergence of Maxwell energy momentum tensor vanishes and that Einstein's equations with cosmological constant are well-defined.

    Asymptotes corresponds to vacuum extremals. In Euclidian regions CP2 type vacuum extremals and in Minkowskian regions to any space-time surface in any 6-D sub-manifold M4× Y2, where Y2 is Lagrangian sub-manifold of CP2 having therefore vanishing induced Kähler form. Symplectic transformations of CP2 combined with diffeomorphisms of M4 give new Lagrangian manifolds. One would expect that vacuum extremals are approached but never reached at second extreme for the flow.

    If one assumes Einstein's equations with a cosmological term, allowed vacuum extremals must be Einstein manifolds. For CP2 type vacuum extremals this is the case. It is quite possible that these fixed points do not actually exist in Minkowskian sector, and could be replaced with more complex asymptotic behavior such as limit, chaos, or strange attractor.

  2. The flow could be also restricted to the space of preferred extremals. Assuming that Einstein Maxwell equations indeed hold true, the flow equations reduce to

    hklDα jk(x,t) ∂βhl= 1/2(kRαβ -Λ gαβ) .

    Preferred extremals would correspond to a fixed sub-manifold of the general flow in the space of all 4-surfaces.

  3. One can also consider a situation in which jk(x,t) is replaced with jk(h,t) defining a flow in the entire imbedding space. This assumption is probably too restrictive. In this case the equations reduce to


    (Dr jl(x,t)+Dljr)∂αhr∂βhl= kRαβ -Λ gαβ .

    Here Dr denotes covariant derivative. Asymptotia is achieved if the tensor Dkjl+Dkjl becomes orthogonal to the space-time surface. Note for that Killing vector fields of H the left hand side vanishes identically. Killing vector fields are indeed symmetries of also asymptotic states.

It must be made clear that the existence of a continuous flow in the space of preferred extremals might be too strong a condition. Already the restriction of the general Maxwell flow in the space of metrics to solutions of Einstein-Maxwell equations with cosmological term might lead to discretization, and the assumption about reprentability as 4-surface in M4 × CP2 would give a further condition reducing the number of solutions. On the other hand, one might consiser a possibility of a continuous flow in the space of constant Ricci scalar metrics with a fixed 4-volume and having hyperbolic spaces as the most symmetric representative.

B.3. Dissipation, self organization, transition to chaos, and coupling constant evolution

A beautiful connection with concepts like dissipation, self-organization, transition to chaos, and coupling constant evolution suggests itself.

  1. It is not at all clear whether the vacuum extremal limits of the preferred extremals can correspond to Einstein spaces except in special cases such as CP2 type vacuum extremals isometric with CP2. The imbeddability condition defines a constraint force which might well force asymptotically more complex situations such as limit cycles and strange attractors. In ordinary dissipative dynamics an external energy feed is essential prerequisite for this kind of non-trivial self-organization patterns. As a matter fact, the fact that the Kähler action equals to

    In the recent case the external energy feed could be replaced by the constraint forces due to the imbeddability condition. It is not too difficult to imagine that the flow (if it exists!) could define something analogous to a transition to chaos taking place in a stepwise manner for critical values of the parameter t. Alternatively, these discrete values could correspond to those values of t for which the preferred extremal property holds true for a general Maxwell flow in the space of 4-metrics. Therefore the preferred extremals of Kähler action could emerge as one-parameter (possibly discrete) families describing dissipation and self-organization at the level of space-time dynamics.

  2. For instance, one can consider the possibility that in some situations Einstein's equations split into two mutually consistent equations of which only the first one is independent

    xJανJνβ = Rαβ ,
    LK= xJανJνβ= 4Λ ,

    x=1/16παK .

    Note that the first equation indeed gives the second one by tracing. This happens for CP2 type vacuum extremals.

    Kähler action density would reduce to cosmological constant which should have a continuous spectrum if this happens always. A more plausible alternative is that this holds true only asymptotically. In this case the flow equation could not lead arbitrary near to vacuum extremal, and one can think of situation in which LK= 4Λ defines an analog of limiting cycle or perhaps even strange attractor. In any case, the assumption would allow to deduce the asymptotic value of the action density which is of utmost importance from calculational point of view: action would be simply SK= 4Λ V4 and one could also say that one has minimal surface with Λ taking the role of string tension.

  3. One of the key ideas of TGD is quantum criticality implying that Kähler coupling strength is analogous to critical temperature. Second key idea is that p-adic coupling constant evolution represents discretized version of continuous coupling constant evolution so that each p-adic prime would correspond a fixed point of ordinary coupling constant evolution in the sense that the 4-volume characterized by the p-adic length scale remains constant. The invariance of the geometric and thus geometric parameters of hyperbolic 4-manifold under the Kähler flow would conform with the interpretation as a flow preserving scale assignable to a given p-adic prime. The continuous evolution in question (if possible at all!) might correspond to a fixed p-adic prime. Also the hierarchy of Planck constants relates to this picture naturally. Planck constant hbareff=nhbar corresponds to a multi-furcation generating n-sheeted structure and certainly affecting the fundamental group.

  4. One can of course question the assumption that a continuous flow exists. The property of being a solution of Einstein-Maxwell equations, imbeddability property, and preferred extremal property might allow allow only discrete sequences of space-time surfaces perhaps interpretable as orbit of an iterated map leading gradually to a fractal limit. This kind of discrete sequence might be also be selected as preferred extremals from the orbit of Maxwell flow without assuming Einstein-Maxwell equations. Perhaps the discrete p-adic coupling constant evolution could be seen in this manner and be regarded as an iteration so that the connection with fractality would become obvious too.

B.4 Does a 4-D counterpart of thermodynamics make sense?

The interpretation of the Kähler flow in terms of dissipation, the constancy of R, and almost constancy of LK suggest an interpretation in terms of 4-D variant of thermodynamics natural in zero energy ontology (ZEO), where physical states are analogs for pairs of initial and final states of quantum event are quantum superpositions of classical time evolutions. Quantum theory becomes a "square root" of thermodynamics so that 4-D analog of thermodynamics might even replace ordinary thermodynamics as a fundamental description. If so this 4-D thermodynamics should be qualitatively consistent with the ordinary 3-D thermodynamics.

  1. The first naive guess would be the interpretation of the action density LK as an analog of energy density e=E/V3 and that of R as the analog to entropy density s=S/V3.
    The asymptotic states would be analogs of thermodynamical equilibria having constant values of LK and R.

  2. Apart from an overall sign factor ε to be discussed, the analog of the first law de= Tds-pdV/V would be

    dLK = kdR +Λ dV4/V4 .

    One would have the correspondences S→ ε RV4,
    e→ ε LK and k→ T, p→ -Λ. k∝ 1/G indeed appears formally in the role of temperature in Einstein's action defining a formal partition function via its exponent. The analog of second law would state the increase of the magnitude of ε RV4 during the Kähler flow.

  3. One must be very careful with the signs and discuss Euclidian and Minkowskian regions separately. Concerning purely thermodynamic aspects at the level of vacuum functional Euclidian regions are those which matter.

    1. For CP2 type vacuum extremals LK ∝ E2+B2 , R=Λ/k, and Λ are positive. In thermodynamical analogy for ε=1 this would mean that pressure is negative.

    2. In Minkowskian regions the value of R=Λ/k is negative for Λ<0 suggested by the large abundance of 4-manifolds allowing hyperbolic metric and also by cosmological considerations. The asymptotic formula LK= 4Λ considered above suggests that also Kähler action is negative in Minkowskian regions for magnetic flux tubes dominating in TGD inspired cosmology: the reason is that the magnetic contribution to the action density LK∝ E2-B2 dominates.
Consider now in more detail the 4-D thermodynamics interpretation in Euclidian and Minkowskian regions assuming that the the evolution by quantum jumps has Kähler flow as a space-time correlate.

  1. In Euclidian regions the choice ε=1 seems to be more reasonable one. In Euclidian regions -Λ as the analog of pressure would be negative, and asymptotically (that is for CP2 type vacuum extremals) its value would be proportional to Λ ∝ 1/GR2, where R denotes CP2 radius defined by the length of its geodesic circle.

    A possible interpretation for negative pressure is in terms of string tension effectively inducing negative pressure (note that the solutions of the modified Dirac equation indeed assign a string to the wormhole contact). The analog of the second law would require the increase of RV4 in quantum jumps. The magnitudes of LK, R, V4 and Λ would be reduced and approach their asymptotic values. In particular, V4 would approach asymptotically the volume of CP2.

  2. In Minkowskian regions Kähler action contributes to the vacuum functional a phase factor analogous to an imaginary exponent of action serving in the role of Morse function so that thermodynamics interpretation can be questioned. Despite this one can check whether thermodynamic interpretation can be considered. The choice ε=-1 seems to be the correct choice now. -Λ would be analogous to a negative pressure whose gradually decreases. In 3-D thermodynamics it is natural to assign negative pressure to the magnetic flux tube like structures as their effective string tension defined by the density of magnetic energy per unit length. -R≥ 0 would entropy and -LK≥ 0 would be the analog of energy density.

    R=Λ/k and the reduction of Λ during cosmic evolution by quantum jumps suggests that the larger the volume of CD and thus of (at least) Minkowskian space-time sheet the smaller the negative value of Λ.

    Assume the recent view about state function reduction explaining how the arrow of geometric time is induced by the quantum jump sequence defining experienced time. According to this view zero energy states are quantum superpositions over CDs of various size scales but with common tip, which can correspond to either the upper or lower light-like boundary of CD. The sequence of quantum jumps the gradual increase of the average size of CD in the quantum superposition and therefore that of average value of V4. On the other hand, a gradual decrease of both -LK and -R looks physically very natural. If Kähler flow describes the effect of dissipation by quantum jumps in ZEO then the space-time surfaces would gradually approach nearly vacuum extremals with constant value of entropy density -R but gradually increasing 4-volume so that the analog of second law stating the increase of -RV4 would hold true.

  3. The interpretation of -R>0 as negentropy density assignable to entanglement is also possible and is consistent with the interpretation in terms of second law. This interpretation would only change the sign factor ε in the proposed formula. Otherwise the above arguments would remain as such.

Saturday, December 01, 2012

Is it possible to learn TGD?


In an earlier blog discussion Hamed asked about some kind of program for learning TGD in roughly the same manner as I did it myself. I decided to write a brief summary about the basic steps leaving aside the worst side tracks since 35 years means too flat learning curve;-).

I wrote a summary about the very first steps, that is the steps made during the four years before my thesis and related to classical dynamics mostly. I could not avoid mentioning and even briefly explaining notions like the "world of classical worlds" (WCW), quantum TGD, Kähler action, modified Dirac equation, zero energy ontology, etc... since I want to relate the problems that I encountered during the first years of TGD to their solutions which came much later, some of them even during this year. I hope that I find time to write similar summaries about later stages in the evolution of TGD and add them to this text.

This summary does not provide any Golden Road to TGD. I do not even know whether it is possible to learn TGD. And certainly it is much more difficult to passively assimilate ideas of others than to actively discover and develop ideas by one self. The authority of the original discoverer - such as that of Witten's - can help enormously but I do not possess this kind of authority so that I must trust only on the power of the ideas themselves.

Since the text consists of five pages it is more practical to give only a link to the pdf file containing it.