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2003
The nilpotent Dirac formalism has been shown, in previous publications, to generate new physical explanations for aspects of particle physics, with the additional possibility of calculating some of the parameters involved in the Standard Model. The applications so far obtained are summarised, with an outline of some more recent developments.
Using the concept of a rewrite (or substitution / production) system we introduce a computational path to the nilpotent Dirac equation, a form outlined by Rowlands (elsewhere in these proceedings). The system differs from traditional rewrite systems in that the rewrite rules allow new symbols to be added to the initial alphabet. The system starts with just one symbol, representing "nothing", and two fundamental rules, create a process which adds news symbols, and conserve a process that examines the effect of any new symbol on those that currently exist. With each step a new sub-alphabet of an infinite univeral alphabet is created. The system may be implemented iteratively, such that a sequence of algebraic properties is required of the emerging sub-alphabets. We outline one such path that proceeds from "nothing" through conjugation, complexification, and dimensionalisation to a steady state in which no fundamentally new symbol is needed. At this stage the alphabet is congruent with the nilpotent Dirac equation in Rowlands' formulation. We suggested that many ways of implementing the computational path exist and these do not need to be at all complicated.
2014
Nilpotent quantum mechanics has developed over a twenty year period into a uniquely powerful method of relativistic quantum mechanics and quantum field theory, which offers many new results relating to particle physics and other fundamental studies. A review of the developments shows that they produce a coherent and integrated approach to a number of fundamental questions. 2000 Mathematics Subject Classification: 53B40, 53B50, 81Q05, 81R05, 81R25.
2001
The nilpotent version of the Dirac equation is applied to the baryon wavefunction, the strong interaction potential, electroweak mixing, and Dirac and Klein-Gordon propagators. The results are used to interpret a quaternion-vector model of particle structures.
New Dirac Equation from the View Point of Particle, 2012
Solution of the Dirac equation with pseudospin symmetry for a new harmonic oscillatory ring-shaped noncentral potential J. Math. Phys. 53, 082104 (2012) Effect of tensor interaction in the Dirac-attractive radial problem under pseudospin symmetry limit J. Math. Phys. 53, 082101 (2012) Asymptotic stability of small gap solitons in nonlinear Dirac equations J. Math. Phys. 53, 073705 (2012) On Dirac-Coulomb problem in (2+1) dimensional space-time and path integral quantization J. Math. Phys. 53, 063503 (2012) Quasi-exact treatment of the relativistic generalized isotonic oscillator Abstract. According to the classical approach, especially the Lorentz Invariant Dirac Equation, when particles are bound to each other, the interaction term appears as a quantity belonging to the "field". In this work, as a totally new approach, we propose to alter the rest masses of the particles due to their interaction, as much as their respective contributions to the static binding energy. Thus we rewrite and solve the Dirac Equation for the hydrogen atom, and amazingly, obtain practically the same numerical results for the ground states, as those obtained from the Dirac Equation.
2000
A version of the Dirac equation is derived from first principles using a combination of quaternions and multivariate 4-vectors. The nilpotent form of the operators used allows us to derive explicit expressions for the wavefunctions of free fermions, vector bosons, scalar bosons; Bose-Einstein condensates, and baryons;annihilation, creation and vacuum operators; the quantum field integrals; and C, P and T transformations;
Physica Scripta, 2012
This paper reexamines the key aspects of Dirac's derivation of his relativistic equation for the electron in order advance our understanding of the nature of quantum field theory. Dirac's derivation, the paper argues, follows the key principles behind Heisenberg's discovery of quantum mechanics, which, the paper also argues, transformed the nature of both theoretical and experimental physics vis-à-vis classical physics and relativity. However, the limit theory (a crucial consideration for both Dirac and Heisenberg) in the case of Dirac's theory was quantum mechanics, specifically, Schrödinger's equation, while in the case of quantum mechanics, in Heisenberg's version, the limit theory was classical mechanics. Dirac had to find a new equation, Dirac's equation, along with a new type of quantum variables, while Heisenberg, to find new theory, was able to use the equations of classical physics, applied to different, quantum-mechanical variables. In this respect, Dirac's task was more similar to that of Schrödinger in his work on his version of quantum mechanics. Dirac's equation reflects a more complex character of quantum electrodynamics or quantum field theory in general and of the corresponding (high-energy) experimental quantum physics vis-à-vis that of quantum mechanics and the (low-energy) experimental quantum physics. The final section examines this greater complexity and its implications for fundamental physics.
Hadron Physics 2000 - Topics on the Structure and Interaction of Hadronic Systems - Proceedings of the International Workshop, 2001
Exact analytic solutions are found to the Dirac equation for a combination of Lorentz scalar and vector Coulombic potentials with additional non-Coulombic parts. An appropriate linear combination of Lorentz scalar and vector non-Coulombic potentials, with the scalar part dominating, can be chosen to give exact analytic Dirac wave functions.
Advanced Studies in Theoretical Physics
The two-component form of the new Dirac equation is obtained for a zero mass particle using a unitary transformation.
Chinese Physics Letters, 2007
The solutions, in terms of orthogonal polynomials, of Dirac equation with analytically solvable potentials are investigated within a novel formalism by transforming the relativistic equation into a Schrödinger like one. Earlier results are discussed in a unified framework and certain solutions of a large class of potentials are given.
The nilpotent formalism for the Dirac equation, outlined in previous papers,is applied to QED. It is shown that what is usually described as 'renormalization' is effectively a statement of the fact that the nilpotent formulation is automatically second quantized and constrains the field into producing finite values for fundamental quantities.
arXiv: General Physics, 2020
We discuss the structure of the Dirac equation and how the nilpotent and the Majorana operators arise naturally in this context. This provides a link between Kauffman's work on discrete physics, iterants and Majorana Fermions and the work on nilpotent structures and the Dirac equation of Peter Rowlands. We give an expression in split quaternions for the Majorana Dirac equation in one dimension of time and three dimensions of space. Majorana discovered a version of the Dirac equation that can be expressed entirely over the real numbers. This led him to speculate that the solutions to his version of the Dirac equation would correspond to particles that are their own anti-particles. It is the purpose of this paper to examine the structure of this Majorana-Dirac Equation, and to find basic solutions to it by using the nilpotent technique. We succeed in this aim and describe our results.
The Dirac equation is a cornerstone of quantum mechanics that fully describes the behaviour of spin ½ particles. Recently, the energy momentum relationship has been reconsidered such that |E|^2 = |(m0c^ 2)| 2 + |(pc)| 2 has been modified to: |E| 2 = |(m0c^2)|^2-|(pc)|^2 where E is the kinetic energy, moc^2 is the rest mass energy and pc is the wave energy for the spin ½ particle. This has been termed the 'Hamiltonian approach' and with a new starting point, the original Dirac equation has been derived: and the modified covariant form found is where h/2π = c = 1. The behaviour of spin ½ particles is found to be the same as for the original Dirac equation. The Dirac equation will also be expanded by setting the rest energy as a complex number, |(m0c 2)| e^jωt
In the present article exact solutions of the Dirac equation for electric neutral particles with anomalous electric and magnetic moments are presented. Using the algebraic method of separation of variables, the Dirac equation is separated in Cartesian, cylindrical, and spherical coordinates, and exact solutions are obtained in terms of special functions.
The internally superluminal electron model is compared to the Dirac equation solution for a free electron. Some background history of the Dirac equation and physics developments that led up to it are also described.
2012
Solution of the Dirac equation with pseudospin symmetry for a new harmonic oscillatory ring-shaped noncentral potential J. Math. Phys. 53, 082104 Effect of tensor interaction in the Dirac-attractive radial problem under pseudospin symmetry limit J. Math. Phys. 53, 082101 Asymptotic stability of small gap solitons in nonlinear Dirac equations J. Math. Phys. 53, 073705 On Dirac-Coulomb problem in (2+1) dimensional space-time and path integral quantization J. Math. Phys. 53, 063503 Quasi-exact treatment of the relativistic generalized isotonic oscillator Abstract. According to the classical approach, especially the Lorentz Invariant Dirac Equation, when particles are bound to each other, the interaction term appears as a quantity belonging to the "field". In this work, as a totally new approach, we propose to alter the rest masses of the particles due to their interaction, as much as their respective contributions to the static binding energy. Thus we re-write and solve the Dirac Equation for the hydrogen atom, and amazingly, obtain practically the same numerical results for the ground states, as those obtained from the Dirac Equation.
A historical revew of the development of the dirac equation is given emphasising the connections with the principles of quontom mechanics. We argue that a consistent relativistic quantisation demands the building of a multiparticle theory from the outset that is a theory where the particle number is not a constant but can change over time and that because quontom field theory obey's this requirement it has been found to be able to quontise systems subject to the constraints of special relativity.
The Dirac equation has a hidden geometric structure that is made manifest by reformulating it in terms of a real spacetime algebra. This reveals an essential connection between spin and complex numbers with profound implications for the interpretation of quantum mechanics. Among other things, it suggests that to achieve a complete interpretation of quantum mechanics, spin should be identifled with an intrinsic zitterbewegung.
We present various generalizations of the Dirac formalism. The different-parity solutions of the Weinberg's 2(2J + 1)-component equations are found. On this basis, generalizations of the Bargmann-Wigner (BW) formalism are proposed. Relations with modern physics constructs are discussed.
Zenodo (CERN European Organization for Nuclear Research), 2023
The Klein-Gordon equation and the Dirac equation are two important equations in particle physics that describe the behavior of massive and spin-1/2 particles, respectively. The Klein-Gordon equation is a second-order partial differential equation given by (◻ + 2) () = 0 where ◻= is the d'Alembertian operator, m is the particle mass, and ()is the wave function describing the particle. The solutions of the Klein-Gordon equation describe massive, spin-0 particles and are plane waves with a dispersion relation given by 2 = → 2 + 2 where E is the energy and → is the momentum of the particle. On the other hand, the Dirac equation is a firstorder partial differential equation given by (−) () = 0, where is the imaginary unit, are the Dirac matrices, m is the particle mass, and ()is the wave function describing the particle. The solutions of the Dirac equation describe massive, spin-1/2 particles and are plane waves with a dispersion relation given by = ± √ → 2 + 2. The solutions of these equations have important implications for our understanding of quantum field theory and the nature of spacetime. The Klein-Gordon equation is a non-interacting equation that is used to describe scalar fields, while the Dirac equation can handle interactions and is used to describe spin-1/2 particles and their interactions with other particles and fields. The dispersion relation of the Klein-Gordon equation is positive definite, while that of the Dirac equation has both positive and negative energy solutions. The wave function in the Klein-Gordon equation is a scalar field, while the wave function in the Dirac equation is a 4-component spinor field. These differences reflect the different physical properties of the particles described by each equation and have important implications for our understanding of the universe. In conclusion, the Klein-Gordon equation and the Dirac equation are two central equations in particle physics that provide a mathematical framework for describing the behavior of massive and spin-1/2 particles. Their solutions and implications continue to play a central role in our understanding of the universe.
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