April, 2008 PROGRESS IN PHYSICS <strong>Vol</strong>ume 2SPECIAL REPORTNew Approach to Quantum ElectrodynamicsSze Kui NgDepartment <strong>of</strong> Mathematics, Hong Kong Baptist University, Hong Kongand School <strong>of</strong> Engineering and Information Technology, Deakin University, AustraliaE-mail: szekuing@yahoo.com.hkIt is shown that a photon with a specific frequency can be identified with the Dirac magneticmonopole. When a Dirac-Wilson line forms a Dirac-Wilson loop, it is a photon.This loop model <strong>of</strong> photon is exactly solvable. From the winding numbers <strong>of</strong> this loopform<strong>of</strong> photon, we derive the quantization properties <strong>of</strong> energy and electric charge. Anew QED theory is presented that is free <strong>of</strong> ultraviolet divergences. <strong>The</strong> Dirac-Wilsonline is as the quantum photon propagator <strong>of</strong> the new QED theory from which we canderive known QED effects such as the anomalous magnetic moment and the Lamb shift.<strong>The</strong> one-loop computation <strong>of</strong> these effects is simpler and is more accurate than that inthe conventional QED theory. Furthermore, from the new QED theory, we have deriveda new QED effect. A new formulation <strong>of</strong> the Bethe-Salpeter (BS) equation solves thedifficulties <strong>of</strong> the BS equation and gives a modified ground state <strong>of</strong> the positronium. Bythe mentioned new QED effect and by the new formulation <strong>of</strong> the BS equation, a termin the orthopositronium decay rate that is missing in the conventional QED is found,resolving the orthopositronium lifetime puzzle completely. It is also shown that thegraviton can be constructed from the photon, yielding a theory <strong>of</strong> quantum gravity thatunifies gravitation and electromagnetism.1 IntroductionIt is well known that the quantum era <strong>of</strong> physics began withthe quantization <strong>of</strong> energy <strong>of</strong> electromagnetic field, fromwhich Planck derived the radiation formula. Einstein thenintroduced the light-quantum to explain the photoelectric effects.This light-quantum was regarded as a particle calledphoton [1–3]. Quantum mechanics was then developed, usheringin the modern quantum physics era. Subsequently, thequantization <strong>of</strong> the electromagnetic field and the theory <strong>of</strong>Quantum Electrodynamics (QED) were established.In this development <strong>of</strong> quantum theory <strong>of</strong> physics, thephoton plays a special role. While it is the beginning <strong>of</strong> quantumphysics, it is not easy to understand as is the quantummechanics <strong>of</strong> other particles described by the Schrödingerequation. In fact, Einstein was careful in regarding thelight-quantum as a particle, and the acceptance <strong>of</strong> the lightquantumas a particle called photon did not come about untilmuch later [1]. <strong>The</strong> quantum field theory <strong>of</strong> electromagneticfield was developed for the photon. However, such difficulties<strong>of</strong> the quantum field theory as the ultraviolet divergencesare well known. Because <strong>of</strong> the difficulty <strong>of</strong> understandingthe photon, Einstein once asked: “What is the photon?” [1].On the other hand, based on the symmetry <strong>of</strong> the electricand magnetic field described by the Maxwell equation andon the complex wave function <strong>of</strong> quantum mechanics, Diracderived the concept <strong>of</strong> the magnetic monopole, which is hypotheticallyconsidered as a particle with magnetic charge, inanalogy to the electron with electric charge. An importantfeature <strong>of</strong> this magnetic monopole is that it gives the quantization<strong>of</strong> electric charge. Thus it is interesting and importantto find such particles. However, in spite <strong>of</strong> much effort, nosuch particles have been found [4, 5].In this paper we shall establish a mathematical model <strong>of</strong>photon to show that the magnetic monopole can be identifiedas a photon. Before giving the detailed model, let us discusssome thoughts for this identification in the following.First, if the photon and the magnetic monopole are differenttypes <strong>of</strong> elementary quantum particles in the electromagneticfield, it is odd that one type can be derived from theother. A natural resolution <strong>of</strong> this oddity is the identification<strong>of</strong> the magnetic monopole as a photon.<strong>The</strong> quantum field theory <strong>of</strong> the free Maxwell equationis the basic quantum theory <strong>of</strong> photon [6]. This free fieldtheory is a linear theory and the models <strong>of</strong> the quantum particlesobtained from this theory are linear. However, a stableparticle should be a soliton, which is <strong>of</strong> the nonlinear nature.Secondly, the quantum particles <strong>of</strong> the quantum theory<strong>of</strong> Maxwell equation are collective quantum effects in thesame way the phonons which are elementary excitations ina statistical model. <strong>The</strong>se phonons are usually considered asquasi-particles and are not regarded as real particles. Regardingthe Maxwell equation as a statistical wave equation <strong>of</strong>electromagnetic field, we have that the quantum particles inthe quantum theory <strong>of</strong> Maxwell equation are analogous to thephonons. Thus they should be regarded as quasi-photons andhave properties <strong>of</strong> photons but not a complete description <strong>of</strong>photons.In this paper, a nonlinear model <strong>of</strong> photon is established.In the model, we show that the Dirac magnetic monopoleSze Kui Ng. New Approach to Quantum Electrodynamics 15
<strong>Vol</strong>ume 2 PROGRESS IN PHYSICS April, 2008can be identified with the photon with some frequencies. Weprovide a U(1) gauge theory <strong>of</strong> Quantum Electrodynamics(QED), from which we derive photon as a quantum Dirac-Wilson loop W(z; z) <strong>of</strong> this model. This nonlinear loopmodel <strong>of</strong> the photon is exactly solvable and thus may be regardedas a quantum soliton. From the winding numbers <strong>of</strong>this loop model <strong>of</strong> the photon, we derive the quantizationproperty <strong>of</strong> energy in Planck’s formula <strong>of</strong> radiation and thequantization property <strong>of</strong> charge. We show that the quantizationproperty <strong>of</strong> charge is derived from the quantizationproperty <strong>of</strong> energy (in Planck’s formula <strong>of</strong> radiation), whenthe magnetic monopole is identified with photon with certainfrequencies. This explains why we cannot physically find amagnetic monopole. It is simply a photon with a specific frequency.From this nonlinear model <strong>of</strong> the photon, we also constructa model <strong>of</strong> the electron which has a mass mechanismfor generating mass <strong>of</strong> the electron. This mechanism <strong>of</strong> generatingmass supersedes the conventional mechanism <strong>of</strong> generatingmass (through the Higgs particles) and makes hypothesizingthe existence <strong>of</strong> the Higgs particles unnecessary. Thisexplains why we cannot physically find such Higgs particles.<strong>The</strong> new quantum gauge theory is similar to the conventionalQED theory except that the former is not based on thefour dimensional space-time (t; x) but is based on the propertime s in the theory <strong>of</strong> relativity. Only in a later stage in thenew quantum gauge theory, the space-time variable (t; x) isderived from the proper time s through the Lorentz metricds 2 = dt 2 dx 2 to obtain space-time statistics and explainthe observable QED effects.<strong>The</strong> derived space variable x is a random variable in thisquantum gauge theory. Recall that the conventional quantummechanics is based on the space-time. Since the spacevariable x is actually a random variable as shown in the newquantum gauge theory, the conventional quantum mechanicsneeds probabilistic interpretation and thus has a most mysteriousmeasurement problem, on which Albert Einstein onceremarked: “God does not play dice with the universe.” Incontrast, the new quantum gauge theory does not involve thementioned measurement problem because it is not based onthe space-time and is deterministic.Thus this quantumgauge theory resolves the mysterious measurement problem<strong>of</strong> quantum mechanics.Using the space-time statistics, we employ Feynman diagramsand Feynman rules to compute the basic QED effectssuch as the vertex correction, the photon self-energy and theelectron self-energy. In this computation <strong>of</strong> the Feynman integrals,the dimensional regularization method in the conventionalQED theory is also used. Nevertheless, while the conventionalQED theory uses it to reduce the dimension 4 <strong>of</strong>space-time to a (fractional) number n to avoid the ultravioletdivergences in the Feynman integrals, the new QED theoryuses it to increase the dimension 1 <strong>of</strong> the proper time to anumber n less than 4, which is the dimension <strong>of</strong> the spacetime,to derive the space-time statistics. In the new QED theory,there are no ultraviolet divergences, and the dimensionalregularization method is not used for regularization.After this increase <strong>of</strong> dimension, the renormalizationmethod is used to derive the well-known QED effects. Unlikethe conventional QED theory, the renormalization method isused in the new QED theory to compute the space-time statistics,but not to remove the ultraviolet divergences, since theultraviolet divergences do not occur in the new QED theory.From these QED effects, we compute the anomalous magneticmoment and the Lamb shift [6]. <strong>The</strong> computation doesnot involve numerical approximation as does that <strong>of</strong> the conventionalQED and is simpler and more accurate.For getting these QED effects, the quantum photon propagatorW(z; z0 ),which is like a line segment connectingtwo electrons, is used to derive the electrodynamic interaction.(When the quantum photon propagator W(z; z0 ) forms aclosed circle with z = z0 , it then becomes a photon W(z; z).)From this quantum photon propagator, a photon propagator isderived that is similar to the Feynman photon propagator inthe conventional QED theory.<strong>The</strong> photon-loop W(z; z) leads to the renormalized electriccharge e and the mass m <strong>of</strong> electron. In the conventionalQED theory, the bare charge e 0 is <strong>of</strong> less importance than therenormalized charge e, in the sense that it is unobservable. Incontrast, in this new theory <strong>of</strong> QED, the bare charge e 0 andthe renormalized charge e are <strong>of</strong> equal importance. While therenormalized charge e leads to the physical results <strong>of</strong> QED,the bare charge e 0 leads to the universal gravitation constantG. It is shown that e = n e e 0 , where n e is a very large windingnumber and thus e 0 is a very small number. It is furthershown that the gravitational constant G = 2e 2 0 which is thusan extremely small number. This agrees with the fact that theexperimental gravitational constant G is a very small number.<strong>The</strong> relationships, e = n e e 0 and G = 2e 2 0, are a part <strong>of</strong>a theory unifying gravitation and electromagnetism. In thisunified theory, the graviton propagator and the graviton areconstructed from the quantum photon propagator. This constructionleads to a theory <strong>of</strong> quantum gravity. In short, a newtheory <strong>of</strong> quantum gravity is developed from the new QEDtheory in this paper, and unification <strong>of</strong> gravitation and electromagnetismis achieved.In this paper, we also derive a new QED effect from theseagull vertex <strong>of</strong> the new QED theory. <strong>The</strong> conventionalBethe-Salpeter (BS) equation is reformulated to resolve itsdifficulties (such as the existence <strong>of</strong> abnormal solutions [7–32]) and to give a modified ground state wave function <strong>of</strong>the positronium. By the new QED effect and the reformulatedBS equation, another new QED effect, a term in the orthopositroniumdecay rate that is missing in the conventionalQED is discovered. Including the discovered term, the computedorthopositronium decay rate now agrees with the experimentalrate, resolving the orthopositronium lifetime puzzlecompletely [33–52]. We note that the recent resolution <strong>of</strong>16 Sze Kui Ng. New Approach to Quantum Electrodynamics
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