## Path integrals for gauge boson radiation versus path integrals for real particles, and Weyl’s gauge symmetry principle The previous post plus a re-reading of Professor Zee’s Quantum Field Theory in a Nutshell (Princeton, 2003) suggests a new formulation for quantum gravity, the mechanism and mathematical predictions of which were given two posts ago.The sum over histories for real particles is used to work out the path of least action, such as the path of a photon of light which takes the least time to bounce off a mirror.  You can do the same thing for the path of a real electron, or the path of a drunkard’s walk.  The integral tells you the effective path taken by the particle, or the probability of any given path being taken, from many possible paths.

For gauge bosons or vector bosons, i.e., force-mediating radiation, the role of the path integral is no longer to find the probability of a path being taken or the effective path.  Instead, gauge bosons are exchanged over many paths simultaneously.  Hence there are two totally different applications of path integrals we are concerned with:

• Applying the path integral for real particles involves evaluating a lot of paths, most of which are not actually taken (the real particle takes only one of those paths, although as Feynman said, it uses a ‘small core of nearby space’ so it can be affected by both of two slits in a screen, provided those slits are close together, within a transverse wavelength or so, so the small core of paths taken overlap both slits).
• Applying the path integral for gauge bosons involves evaluating a lot of paths which are all actually being taken, because the extensive force field is composed of lots of gauge bosons being exchanged between charges, really going all over the place (for long-range gravity and electromagnetism).

In both cases the path taken by a given real particle or a single gauge boson must be composed of straight lines in between interactions (see Fig. 1 of previous post) because the curvature of general relativity appears to be a classical approximation to a lot of small discrete deflections due to discrete interactions with field quanta (sometimes curves are used in Feynman diagrams for convenience, but according to quantum field theory all mechanisms for curvature actually involve lots of little deflections by the quanta of fields).

The calculations of quantum gravity, two posts ago, use geometry to evaluate these straight-line gauge boson paths for gravity and electromagnetism.  Presumably, translating the simplicity of the calculations based on geometry in that post into a path integrals will appeal more to the stringy mainstream.  Loop quantum gravity methods of summing up a lot of interaction graphs will be used to do this.  What is vital are directional asymmetries, which transform a perfect symmetry of gauge boson exchanges in all directions into a force, represented by the geometry of Fig. 1 (below).  One way to convert that geometry into a formula is to consider the inward-outward travelling isotropic graviton exchange radiation by using divergence operator.  I think this can be done easily because there are two useful physical facts which make the geometry simpler even than appears from Fig. 1: first, the shield area x in Fig. 1 is extremely small so the asymmetry cone can not ever have a large sized base for any practical situation; second, by Newton’s proof the gravity inverse square law force from a lot of little particles spread out in the Earth is the same as you get by mathematically assuming that all the little masses (fundamental particles) are not spread throughout a large planet but are all at the centre.  So a path integral formulation for the geometry of Fig. 1 is simple. Fig. 1: Mechanism for quantum gravity (a tiny falling test mass is located in the middle of the universe, which experiences isotropic graviton radiation –  spin 1 gravitons which cause attraction by simply pushing things as this allows predictions as proved in the earlier post – from all directions except that where there is an asymmetry produced by the mass which shields that radiation). By Newton’s 3rd law the outward force of the big bang has an equal inward force, and gravity is equal to the proportion of that inward force covered by the shaded cone in this diagram: (force of gravity) = (total inward force).(cross sectional area of shield projected out to radius R, i.e., the area of the base of the cone marked x, which is the product of the shield’s cross-sectional area and the ratio R2/r2) / (total spherical area with radius R).  (Full proof here.)

Weyl’s gauge symmetry principle

A symmetry is anything that doesn’t change as the result of a transformation.  For example, the colour of a plastic pen doesn’t change when you rotate it, so the colour is a symmetry of the pen when the transformation type is a rotation.  If you transform the plastic pen by burning it, colour is not a symmetry of the pen (unless the pen was the colour of carbon in the first place).

A gauge symmetry is one where scalable quantities (gauges) are involved.  For example, there is a symmetry in the fact that the same amount of energy is required to lift a 1 kg mass up by a height of 1 metre, regardless of the original height of the mass above sea level.  (This example is not completely true, but it is almost true because the fall in gravity acceleration with height is small, as gravity is only 0.3% weaker at the top of the tallest mountain than it is at sea level.)

The female mathematician Emmy Noether in 1915 proved a great theorem which states that any continuous symmetry leads to a conservation law, e.g., the symmetry of physical laws (due to these laws remaining the same while time passes) leads to the principle of conservation of energy!  This particularly impressive example of Noether’s theorem does not strictly apply to forces over very long time scales, because, as proved, fundamental force coupling constants (relative charges) increase in direct proportion to the age of the universe.  However, the theorem is increasingly accurate as the time scale involved is reduced and the inaccuracy becomes trivial when the time considered is small compared to the age of the universe.

At the end of Quantum Field Theory in a Nutshell (at page 457), Zee points out that Maxwell’s equations unexpectedly contained two hidden symmetries, Lorentz invariance and gauge invariance: ‘two symmetries that, as we now know, literally hold the key to the secrets of the universe.’

He then argues that Maxwell’s long-hand differential equations masked these symmetries and it took Einstein’s genius to uncover them (special relativity for Lorentz invariance, general relativity for the tensor calculus with the repeated-indices summation convention, e.g., mathematical symbol compressions by defining notation which looks something like: Fab = 2dAab = daAb – dbAa).  This is actually a surprisingly good point to make.

Zee, judging from what his Quantum Field Theory in a Nutshell book contains, does not seem to be aware how useful Heaviside’s vector calculus is (Heaviside compressed Maxwell’s 20 equations into 4 field equations plus a continuity equation for conservation of charge, while Einstein merely compressed the 4 field equations into 2, a less impressive feat but one leading to less intuitive equations; divergence and curl equations in vector calculus describe simple divergence of radial electric field lines which you can picture, and simple curling of electric or magnetic field lines which again are easy to picture).  In addition, the way relativity comes from Maxwell’s equations is best expressed non-mathematically, just because it is so simple: if you move relative to an electric charge you get a magnetic field, if you don’t move relative to an electric charge you don’t see the magnetic field.

Zee adds: ‘it is entirely possible that an insightful reader could find a hitherto unknown symmetry hidden in our well-studied field theories.’

Just to be absolutely lucid on this, so that there can be no possible confusion:

• SU(2) correctly asserts that quarks form quark-antiquark doublets due to the short-range weak force mediated by massive weak gauge bosons
• U(1) falsely asserts that leptons do not form doublets due to the long-range electromagnetic force mediated by mass-less electromagnetic gauge bosons.

The correct picture to replace SU(2)xU(1) is based on the same principle for SU(2) but a replacement of U(1) by another effect of SU(2):

• SU(2) correctly asserts that quarks form quark-antiquark doublets due to the short-range weak force mediated by massive weak gauge bosons.
• SU(2) also correctly asserts that leptons form lepton-antilepton doublets (although since the binding force is long-range electromagnetism instead of short-range massive weak gauge bosons, the lepton-antilepton doublets are not confined in a small place because the range over which the electromagnetic force operates is simply far greater than that of the weak force).

Solid experimentally validated evidence for this (including mechanisms and predictions of gravity and electromagnetism strengths, etc., from massless SU(2) gauge boson interactions which automatically explain gravity and electromagnetism): here.  Sheldon Glashow’s early expansion of the original Yang-Mills SU(2) gauge interaction symmetry to unify electromagnetism and weak interactions is quoted here.  More technical discussion on the relationship of leptons to quarks implies by the model: here.

However, innovation of a checkable sort is now unwelcome in mainstream stringy physics, so maybe Zee was joking, and maybe he secretly doesn’t want any progress (unless of course it comes from mainstream string theory).  This suggestion is made because Zee on the same page (p457) adds that the experimentally-based theory of electromagnetic unification (unification of electricity and magnetism) was a failure to achieve its full potential because those physicists: ‘did not possess the mind-set for symmetry.  The old paradigm “experiments -> action -> symmetry” had to be replaced in fundamental physics by the new paradigm “symmetry -> action -> experiments,” the new paradigm being typified by grand unified theory and later by string theory.’  (Emphasis added.)

Problem is, string theory has proved an inedible, stinking turkey (Lunsford both more politely and more memorably calls string ‘a vile and idiotic lie’ which ‘has managed to slough itself along for 20 years, leaving a shiny trail behind it’).  I’ve explained politely why string theory is offensive, insulting, abusive, dictatorial ego-massaging, money-laundering pseudoscience at my domain http://quantumfieldtheory.org/.

Zee needs to try reading Paul Feyerabend’s book, Against Method.  Science actually works by taking the route that most agrees with nature, regardless of how unorthodox an idea is, or how crazy it superficially looks to the prejudiced who don’t bother to check it objectively before arriving at a conclusion on its merits; ‘science,’ when it does occasionally take the popular route that is a total and complete moronic failure, e.g., mainstream string, temporarily becomes a religion.  String theorists are like fanatical preachers, trying to dictate to the gullible what nature is like ahead of any evidence, the very error Bohr alleged Einstein was making in 1927.  Actually there is a strong connection between the speculative Copenhagen Interpretation propaganda of Bohr in 1927 (Bohr in fact had no solid evidence for his pet theory of metaphysics, while Einstein had every causal law and mechanism of physics on his side; today we all know from high-energy physics that virtual particles are an experimental physics fact and they cause indeterminancy in a simple mechanical way on small distance scales), and string.  Both rely on exactly the same mixture of lies, hype, coercion, ridicule of factual evidence, etc.  Both are religions.  Neither is a science, and no matter how much physically vacuous mathematical obfuscation they use, it’s failure to cover-up the gross incompetence in basic physics remains as perfectly transparent as the Emperor’s new clothes.  Unfortunately, most people see what they are told to see, so this farce of string theory continues.

## 9 thoughts on “Path integrals for gauge boson radiation versus path integrals for real particles, and Weyl’s gauge symmetry principle”

1. Nigel Cook says:

copy of a comment:

“Theoretically if an accelerator fired enough mass into a tiny space a singularity would be created. The Black Hole would almost instantly evaporate, but could be detected via Hawking radiation. Unfortunately quantum mechanics says that a particle’s location can not be precisely measured. This quantum uncertainty would prevent us from putting enough mass into a singularity.”

I disagree with Lisa Randall here. It depends on whether the black hole is charged or not, which changes the mechanism for the emission of Hawking radiation.

The basic idea is that in a strong electric field, pairs of virtual positive fermions and virtual negative fermions appear spontaneously. If this occurs at the event horizon of a black hole, one of the pair can at random fall into the black hole, while the other one escapes.

However, there is a factor Hawking and Lisa Randall ignore: the requirement of the black hole having electric charge in the first place, because pair production has only been demonstrated to occur in strong fields, the standard model fields of the strong and electromagnetic force fields (nobody has ever seen pair production occur in the extremely weak gravitational fields).

Hawking ignores the fact that pair production in quantum field theory (according to Schwinger’s calculations, which very accurately predict other things like the magnetic moments of leptons and the Lamb shift in the hydrogen spectra) requires a net electric field to exist at the event horizon at the black hole.

This in turn means that the black hole must carry a net electric charge and cannot be neutral if there is to be any Hawking radiation.

In turn, this implies that Hawking radiation in general is not gamma rays as Hawking claims it is.

Gamma rays in Hawking’s theory are produced just beyond the event horizon of the black hole by as many virtual positive fermions as virtual negative fermions escaping and then annihilating into gamma rays.

This mechanism can’t occur if the black hole is charged, because the net electric charge [which is required to give the electric field which is required for pair-production in the vacuum in the first place] of the black hole interferes with the selection of which virtual fermions escape from the event horizon!

If the black hole has a net positive charge, it will skew the distribution of escaping radiation so that more virtual positive charges escape than virtual negative charges.

This, in turn, means that the escaped charges beyond the event horizon won’t be equally positive and negative; so they won’t be able to annihilate into gamma rays.

It’s strange that Hawking has never investigated this.

You only get Hawking radiation if the black hole has an electric charge of Q > 16*Pi*Permittivity*[(mMG)^2]/(c*e*h-bar).

(This condition is derived below.)

The type of Hawking radiation you get emitted is generally going to be charged, not neutral.

My understanding is that the fermion and boson are both results of fundamental prions. As Carl Brannen and Tony Smith have suggested, fermions may be a triplet of prions to explain the three generations of the standard model, and the colour charge in SU(3) QCD.

Bosons of the classical photon variety would generally have two prions: because their electric field oscillates from positive to negative (the positive electric field half cycle constitutes an effective source of positive electric charge and can be considered to be one preon, while the negative electric field half cycle in a photon can be considered another preon).

Hence, there are definite reasons to suspect that all fermions are composed of three preons, while bosons consist of pairs of preons.

Considering this, Hawking radiation is more likely to be charged gauge boson radiation. This does explain electromagnetism if you replace the U(1)xSU(2) electroweak unification with an SU(2) electroweak unification, where you have 3 gauge bosons which exist in both massive forms (at high energy, mediating weak interactions) and also massless forms (at all energies), due to the handedness of the way these three gauge bosons acquire mass from a mass-providing field. Since the standard model’s electroweak symmetry breaking (Higgs) field fails to make really convincing falsifiable predictions (there are lots of versions of Higgs field ideas making different “predictions”, so you can’t falsify the idea easily), it is very poor physics.

Sheldon Glashow and Julian Schwinger investigated the use of SU(2) to unify electromagnetism and weak interactions in 1956, as Glashow explains in his Nobel lecture of 1979:

‘Schwinger, as early as 1956, believed that the weak and electromagnetic interactions should be combined into a gauge theory. The charged massive vector intermediary and the massless photon were to be the gauge mesons. As his student, I accepted his faith. … We used the original SU(2) gauge interaction of Yang and Mills. Things had to be arranged so that the charged current, but not the neutral (electromagnetic) current, would violate parity and strangeness. Such a theory is technically possible to construct, but it is both ugly and experimentally false [H. Georgi and S. L. Glashow, Physical Review Letters, 28, 1494 (1972)]. We know now that neutral currents do exist and that the electroweak gauge group must be larger than SU(2).’

This is plain wrong: Glashow and Schwinger believed that electromagnetism would have to be explained by a massless uncharged photon acting as the vector boson which communicates the force field.

If they had considered the mechanism for how electromagnetic interactions can occur, they would have seen that it’s entirely possible to have massless charged vector bosons as well as massive ones for short range weak force interactions. Then SU(2) gives you six vector bosons:

Massless W_+ = +ve electric fields
Massless W_- = -ve electric fields
Massless Z_o = graviton (neutral)

Massive W_+ = mediates weak force
Massive W_- = mediates weak force
Massive Z_o = neutral currents

Going back to the charged radiation from black holes, massless charged radiation mediates electromagnetic interactions.

This idea that black holes must evaporate if they are real simply because they are radiating, is flawed: air molecules in my room are all radiating energy, but they aren’t getting cooler: they are merely exchanging energy. There’s an equilibrium.

Equations

To derive the condition for Hawking’s heuristic mechanism of radiation emission, he writes that pair production near the event horizon sometimes leads to one particle of the pair falling into the black hole, while the other one escapes and becomes a real particle. If on average as many fermions as antifermions escape in this manner, they annihilate into gamma rays outside the black hole.

Schwinger’s threshold electric field for pair production is: E_c = (m^2)*(c^3)/(e*h-bar) = 1.3*10^18 volts/metre. Source: equation 359 in http://arxiv.org/abs/quant-ph/0608140 or equation 8.20 in http://arxiv.org/abs/hep-th/0510040

So at least that electric field strength must exist at the event horizon, before black holes emit any Hawking radiation! (This is the electric field strength at 33 fm from an electron.) Hence, in order to radiate by Hawking’s suggested mechanism, black holes must carry enough electric charge so make the eelectric field at the event horizon radius, R = 2GM/c^2, exceed 1.3*10^18 v/m.

Now the electric field strength from an electron is given by Coulomb’s law with F = E*q = qQ/(4*Pi*Permittivity*R^2), so

E = Q/(4*Pi*Permittivity*R^2) v/m.

Setting this equal to Schwinger’s threshold for pair-production, (m^2)*(c^3)/(e*h-bar) = Q/(4*Pi*Permittivity*R^2). Hence, the maximum radius out to which fermion-antifermion pair production and annihilation can occur is

R = [(Qe*h-bar)/{4*Pi*Permittivity*(m^2)*(c^3)}]^{1/2}.

Where Q is black hole’s electric charge, and e is electronic charge, and m is electron’s mass. Set this R equal to the event horizon radius 2GM/c^2, and you find the condition that must be satisfied for Hawking radiation to be emitted from any black hole:

Q > 16*Pi*Permittivity*[(mMG)^2]/(c*e*h-bar)

where M is black hole mass.

So the amount of electric charge a black hole must possess before it can radiate (according to Hawking’s mechanism) is proportional to the square of the mass of the black hole.

On the other hand, it’s interesting to look at fundamental particles in terms of black holes (Yang-Mills force-mediating exchange radiation may be Hawking radiation in an equilibrium).

When you calculate the force of gauge bosons emerging from an electron as a black hole (the radiating power is given by the Stefan-Boltzmann radiation law, dependent on the black hole radiating temperature which is given by Hawking’s formula), you find it correlates to the electromagnetic force, allowing quantitative predictions to be made. See https://nige.wordpress.com/2007/05/25/quantum-gravity-mechanism-and-predictions/#comment-1997 for example.

To summarize: Hawking, considering uncharged black holes, says that either of the fermion-antifermion pair is equally likey to fall into the black hole. However, if the black hole is charged (as it must be in the case of an electron), the black hole charge influences which particular charge in the pair of virtual particles is likely to fall into the black hole, and which is likely to escape. Consequently, you find that virtual positrons fall into the electron black hole, so an electron (as a black hole) behaves as a source of negatively charged exchange radiation. Any positive charged black hole similarly behaves as a source of positive charged exchange radiation.

These charged gauge boson radiations of electromagnetism are predicted by an SU(2) electromagnetic mechanism, see Figures 2, 3 and 4 of https://nige.wordpress.com/2007/06/20/the-mathematical-errors-in-the-standard-model-of-particle-physics/

It’s amazing how ignorant mainstream people are about this. They don’t understand that charged massless radiation can only propagate if there is an exchange (vector boson radiation going in both directions between charges) so that the magnetic field vectors cancel, preventing infinite self inductance.

Hence the whole reason why we can only send out uncharged photons from a light source is that we are only sending them one way. Feynman points out clearly that there are additional polarizations but observable long-range photons only have two polarizations.

It’s fairly obvious that between two positive charges you have a positive electric field because the exchanged vector bosons which create that field are positive in nature. They can propagate despite being massless because there is a high flux of charged radiation being exchanged in both directions (from charge 1 to charge 2, and from charge 2 to charge 1) simultaneously, which cancels out the magnetic fields due to moving charged radiation and prevents infinite self-inductance from stopping the radiation. The magnetic field created by any moving charge has a directional curl, so radiation of similar charge going in opposite directions will cancel out the magnetic fields (since they oppose) for the duration of the overlap.

All this is well known experimentally from sending logic signals along transmission lines, which behave as photons. E.g. you need two parallel conductors at different potential to cause a logic signal to propagate, each conductor containing a field waveform which is an exact inverted image of that in the other (the magnetic fields around each of the conductors cancels the magnetic field of the other conductor, preventing infinite self-inductance).

Moreover, the full mechanism for this version of SU(2) makes lots of predictions. So fermions are blac[k] holes and the charged Hawking radiation they emit is the gauge bosons of electromagnetism and weak interactions.

Presumably the neutral radiation is emitted by electrically neutral field quanta which give rise to the mass (gravitational charge). The reason why gravity is so weak is because it is mediated by electrically neutral vector bosons.