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A Wave Equation including Leptons and Quarks for the Standard Model of Quantum Physics in Clifford Algebra 被引量:1
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2014年第18期2149-2173,共25页
A wave equation with mass term is studied for all fermionic particles and antiparticles of the first generation: electron and its neutrino, positron and antineutrino, quarks u and d with three states of color and anti... A wave equation with mass term is studied for all fermionic particles and antiparticles of the first generation: electron and its neutrino, positron and antineutrino, quarks u and d with three states of color and antiquarks and . This wave equation is form invariant under the group generalizing the relativistic invariance. It is gauge invariant under the U(1)×SU(2)×SU(3) group of the standard model of quantum physics. The wave is a function of space and time with value in the Clifford algebra Cl1,5. Then many features of the standard model, charge conjugation, color, left waves, and Lagrangian formalism, are obtained in the frame of the first quantization. 展开更多
关键词 Invariance Group Dirac Equation Electromagnetism Weak INTERACTIONS Strong INTERACTIONS CLIFFORD ALGEBRAS
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Three Clifford Algebras for Four Kinds of Interactions 被引量:1
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2016年第9期936-951,共16页
Three Clifford algebras are sufficient to describe all interactions of modern physics: The Clifford algebra of the usual space is enough to describe all aspects of electromagnetism, including the quantum wave of the e... Three Clifford algebras are sufficient to describe all interactions of modern physics: The Clifford algebra of the usual space is enough to describe all aspects of electromagnetism, including the quantum wave of the electron. The Clifford algebra of space-time is enough for electro-weak interactions. To get the gauge group of the standard model, with electro-weak and strong interactions, a third algebra is sufficient, with only two more dimensions of space. The Clifford algebra of space allows us to include also gravitation. We discuss the advantages of our approach. 展开更多
关键词 GEOMETRY Invariance Group Dirac Equation Electromagnetism Weak Interactions Strong Interactions Clifford Algebras GRAVITATION
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Towards the Unification, Part 2: Simplified Equations, Covariant Derivative, Photons 被引量:1
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作者 Claude Daviau Jacques Bertrand Dominique Girardot 《Journal of Modern Physics》 2016年第16期2398-2417,共21页
We continue the study of the Standard Model of Quantum Physics in the Clifford algebra of space. We get simplified mass terms for the fermion part of the wave. We insert the simplified equations in the frame of Genera... We continue the study of the Standard Model of Quantum Physics in the Clifford algebra of space. We get simplified mass terms for the fermion part of the wave. We insert the simplified equations in the frame of General Relativity. We construct the electromagnetic field of the photon, alone boson without proper mass. We explain how the Pauli principle comes from the equivalence principle of General Relativity. We transpose in the frame of the algebra of space the second quantification of the electromagnetic field. We discuss the changes introduced here. 展开更多
关键词 BOSON Clifford Algebra Dirac Equation Electromagnetism Electron GRAVITATION Magnetic Monopole Neutrino Photon QUARK Relativistic Invariance Strong Interactions Weak Interactions
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Geometry of the Standard Model of Quantum Physics
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作者 Claude Daviau Jacques Bertrand 《Journal of Applied Mathematics and Physics》 2015年第1期46-61,共16页
General relativity links gravitation to the structure of our space-time. Nowadays physics knows four types of interactions: Gravitation, electromagnetism, weak interactions, strong interactions. The theory of everythi... General relativity links gravitation to the structure of our space-time. Nowadays physics knows four types of interactions: Gravitation, electromagnetism, weak interactions, strong interactions. The theory of everything (ToE) is the unification of these four domains. We study several necessary cornerstones for such a theory: geometry and mathematics, adapted manifolds on the real domain, Clifford algebras over tangent spaces of these manifolds, the real Lagrangian density in connection with the standard model of quantum physics. The geometry of the standard model of quantum physics uses three Clifford algebras. The algebra ?of the 3-dimensional physical space is sufficient to describe the wave of the electron. The algebra of space-time is sufficient to describe the wave of the pair electron-neutrino. A greater space-time with two additional dimensions of space generates the algebra . It is sufficient to get the wave equation for all fermions, electron, its neutrino and quarks u and d of the first generation, and the wave equations for the two other generations. Values of these waves allow defining, in each point of space-time, geometric transformations from one intrinsic manifold of space-time into the usual manifold. The Lagrangian density is the scalar part of the wave equation. 展开更多
关键词 GEOMETRY of the STANDARD MODEL of QUANTUM PHYSICS
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Relativistic Gauge Invariant Wave Equation of the Electron-Neutrino
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2014年第11期1001-1022,共22页
With the right and the left waves of an electron, plus the left wave of its neutrino, we write the tensorial densities coming from all associations of these three spinors. We recover the wave equation of the electro-w... With the right and the left waves of an electron, plus the left wave of its neutrino, we write the tensorial densities coming from all associations of these three spinors. We recover the wave equation of the electro-weak theory. A new non linear mass term comes out. The wave equation is form invariant, then relativistic invariant, and it is gauge invariant under the U(1)×SU(2), Lie group of electro-weak interactions. The invariant form of the wave equation has the Lagrangian density as real scalar part. One of the real equations equivalent to the invariant form is the law of conservation of the total current. 展开更多
关键词 INVARIANCE Group Dirac Equation Weak Interactions GAUGE INVARIANCE Electron NEUTRINO CLIFFORD ALGEBRAS Magnetic MONOPOLE
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Left Chiral Solutions for the Hydrogen Atom of the Wave Equation for Electron + Neutrino
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2015年第11期1647-1656,共10页
The resolution of our wave equation for electron + neutrino is made in the case of the H atom. From two non-classical potentials, we get chiral solutions with the same set of quantum numbers and the same energy levels... The resolution of our wave equation for electron + neutrino is made in the case of the H atom. From two non-classical potentials, we get chiral solutions with the same set of quantum numbers and the same energy levels as those coming from the Dirac equation for the lone electron. These chiral solutions are available for each electronic state in any atom. We discuss the implications of these new potentials. 展开更多
关键词 Hydrogen Atom Quantum Numbers Energy Levels CHIRALITY ELECTRON NEUTRINO Electro-Weak GAUGE
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Extended Relativistic Invariance, Quantization of the Kinetic Momentum
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2020年第9期1263-1278,共16页
The aim of this research is a better understanding of the quantization in physics. The true origin of the quantization is the existence of the quantized kinetic momentum of electrons, neutrinos, protons and neutrons w... The aim of this research is a better understanding of the quantization in physics. The true origin of the quantization is the existence of the quantized kinetic momentum of electrons, neutrinos, protons and neutrons with the <img src="Edit_6224bcbf-d22a-433a-9554-e7b4c49743ed.bmp" alt="" /> value. It is a consequence of the extended relativistic invariance of the wave of fundamental particles with spin 1/2. This logical link is due to properties of the quantum waves of fermions, which are functions of space-time with value into the <img src="Edit_21be84cf-f75c-41c3-ba66-4067f1da843a.bmp" alt="" /> and End(<em>Cl</em><sub>3</sub>) Lie groups. Space-time is a manifold forming the auto-adjoint part of <img src="Edit_b4b9925e-1f73-4305-b3ba-060a6186ffb0.bmp" alt="" />. The Lagrangian densities are the real parts of the waves. The equivalence between the invariant form and the Dirac form of the wave equation takes the form of Lagrange's equations. The momentum-energy tensor linked by Noether's theorem to the invariance under space-time translations has components which are directly linked to the electromagnetic tensor. The invariance under <img src="Edit_b4b9925e-1f73-4305-b3ba-060a6186ffb0.bmp" alt="" style="white-space:normal;" /> of the kinetic momentum tensor gives eight vectors. One of these vectors has a time component with value <img src="Edit_6224bcbf-d22a-433a-9554-e7b4c49743ed.bmp" alt="" style="white-space:normal;" />. Resulting aspects of the standard model of quantum physics and of the relativistic theory of gravitation are discussed. 展开更多
关键词 Geometry Invariance Group Dirac Equation Electromagnetism Weak Interactions Strong Interactions Clifford Algebras GRAVITATION QUANTIZATION
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Electro-Weak Gauge, Weinberg-Salam Angle
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2015年第14期2080-2092,共13页
The main aim of this paper is to explain why the Weinberg-Salam angle in the electro-weak gauge group satisfies . We study the gauge potentials of the electro-weak gauge group from our wave equation for electron + neu... The main aim of this paper is to explain why the Weinberg-Salam angle in the electro-weak gauge group satisfies . We study the gauge potentials of the electro-weak gauge group from our wave equation for electron + neutrino. These potentials are space-time vectors whose components are amongst the tensor densities without derivative built from the three chiral spinors of the wave. The ?gauge invariance allows us to identify the four potential space-time vectors of the electro-weak gauge to four of the nine possible vectors. One and only one of the nine derived bivector fields is the massless electromagnetic field. Putting back the four potentials linked to the spinor wave into the wave equation we get simplified equations. From the properties of the second-order wave equation we obtain the Weinberg-Salam angle. We discuss the implications of the simplified equations, obtained without second quantification, on mass, charge and gauge invariance. Chiral gauge, electric gauge and weak gauge are simply linked. 展开更多
关键词 Invariance Group Dirac Equation Chirality Electron Neutrino Electro-Weak GAUGE GAUGE Bosons Photon Weinberg-Salam Angle
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Including Space-Time in the Extended Group Cl3* of Relativistic Form-Invariance
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 CAS 2022年第8期1147-1156,共10页
The inclusion of space-time in the extended group of relativistic form-invariance, Cl<sub>3</sub>*</sup>, is specified as the inclusion of the whole space-time manifold in this multiplicative Lie gro... The inclusion of space-time in the extended group of relativistic form-invariance, Cl<sub>3</sub>*</sup>, is specified as the inclusion of the whole space-time manifold in this multiplicative Lie group. First physical results presented here are: the geometric origin of the time arrow, a better understanding of the non-simultaneity in optics and a mainly geometric origin for the universe expansion, and its recent acceleration. 展开更多
关键词 Space-Time Manifold Invariance Group Standard Model Acceleration of Expansion
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Scientific Community and Remaining Errors, Physics Examples
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作者 Claude Daviau Jacques Bertrand 《Journal of Modern Physics》 2018年第2期250-258,共9页
The scientific community controls the possible errors by a rigorous process using referees. Consequently the only possible errors are very few, they come from what anyone considers obviously true. Three of these error... The scientific community controls the possible errors by a rigorous process using referees. Consequently the only possible errors are very few, they come from what anyone considers obviously true. Three of these errors are pointed here: the main one is the belief that any quantum state follows a Schr&ouml;dinger equation. This induces two secondary errors: the impossibility of magnetic charges and the identification between the Lorentz group and SL (2, C). 展开更多
关键词 Invariance Group Schrodinger Equation Dirac Equation Electromagnetism Weak Interactions Strong Interactions Clifford Algebra Magnetic Monopole
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Towards the Unification of All Interactions (The First Part: The Spinor Wave)
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作者 Claude Daviau Jacques Bertrand Dominique Girardot 《Journal of Modern Physics》 2016年第12期1568-1590,共23页
For the unification of gravitation with electromagnetism, weak and strong interactions, we use a unique and very simple framework, the Clifford algebra of space . We enlarge our previous wave equation to the general c... For the unification of gravitation with electromagnetism, weak and strong interactions, we use a unique and very simple framework, the Clifford algebra of space . We enlarge our previous wave equation to the general case, including all leptons, quarks and antiparticles of the first generation. The wave equation is a generalization of the Dirac equation with a compulsory non-linear mass term. This equation is form invariant under the group of the invertible elements in the space algebra. The form invariance is fully compatible with the gauge invariance of the standard model. The wave equations of the different particles come by Lagrange equations from a Lagrangian density and this Lagrangian density is the sum of the real parts of the wave equations. Both form invariance and gauge invariance are exact symmetries, not only partial or broken symmetries. Inertia is already present in the part of the gauge group and the inertial chiral potential vector simplifies weak interactions. Relativistic quantum physics is then a naturally yet unified theory, including all interactions. 展开更多
关键词 Electromagnetism Weak Interactions Strong Interactions GRAVITATION Clifford Algebra Dirac Equation Lagrangian Formalism Gauge Groups Relativistic Invariance Electron Magnetic Monopole QUARK Photon Gauge Boson Unification
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