On Generalized Dirac's Equation

Delso J

Bachelor's Degree in Physics by Zaragoza University, Spain

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Abstract

In four dimensions, the Minkowski metric leads to the 16 dimensional Clifford algebra C(1,3), Dirac equation is using four of these 16 matrices that form a basis of this algebra, a new operator is defined using all of these matrices and also generalized for a curved space

Multilevel operator

We are using Pauli matrices σ, electromagnetic four-potential Aμ and charge e with [1].

                                                                                                            (1)

In four dimensions, Minkowski's metric leads to the Clifford algebra C Dirac matrices

                                                                   (2)

Multilevel operator Dn acts on level n, n is the number of matrices in the product of the algebra members, for example, D3 acts on . Total multilevel operator Dmul = D0 +D1 +D2 +D3 +D4, the action of Dmul on the spinor function vanishes

                                                                                                                                                                                                   (4)

                                                                                                                                                                               (5)

                                                                                                                                           (6)

                                                                                                                                                                                  (7)

                                                                       (8)

                                                   (9)

Multilevel operator Dmul(ημν ,Aμ ,e) can be generalized for a curved space with four-potential P, field charge q and covariant derivative[3] (;μ) instead of derivative (,μ) in the definition of

                                                                                                                                                                           (10)

                                                                                                                                                                               (11)

                                                                                                                                                                                                  (12)

                                                                                                                                                                               (13)

                                                                                                                                         (14)

                                                                                                                                       (15)

                                                                                                                                                                     (16)

                                                                                                                                  (17)

For gravity is the new gravitomagnetic tensor. is the torsion tensor [4].

with                                                                                                                         (18)

with the Riemann-Christoffel tensor [5].                                                                                                (19)

                                                                (20)

with                                                                                                            (21)

                                                                                                                                                         (22)

                                                                                                                     (23)

Conclusions

Multilevel operator has been generalized for a curved space with a general four-potential P. For gravity is the new gravitomagnetic tensor and torsion tensor appears in its definition.

In a flat space and operators vanish. In a curved space the curvature tensor appears in levels 3 and 4.

The appearance of torsion tensor and curvature tensor in multilevel operator means that this operator is a fundamental operator in Quantum Field Theory.

References

  1. Marian Fecko (2006) Differential Geometry and Lie Groups for Physicists. Cambridge University Press 637.
  2. Marian Fecko (2006) Differential Geometry and Lie Groups for Physicists. Cambridge University Press 650-652. 
  3. Marian Fecko (2006) Differential Geometry and Lie Groups for Physicists. Cambridge University Press 380. 
  4. Marian Fecko (2006) Differential Geometry and Lie Groups for Physicists. Cambridge University Press 384. 
  5. Marian Fecko (2006 Differential Geometry and Lie Groups for Physicists. Cambridge University Press 404.
Editorial Information

Article Type

Short Communication

Publication history

Received date: January 15, 2022
Accepted date: January 21, 2023
Published date: January 31, 2023

Copyright

©2023 Delso J. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

Citation

Delso J (2023) On Generalized Dirac's Equation. OSP Journal of Physics and Astronom 4: JPA-4-142.

Corresponding author

Jesus Delso Lapuerta

Bachelor's Degree in Physics by Zaragoza University, Spain. jesus.delso@gmail.com

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