The free particle solutions of the relativistic Dirac equation are characterized by plane waves with infinite uncertainty in position. However, many practical implementations of the solutions require a wave packet configuration, which can be utilized to represent a localized Dirac particle. Unlike the traditional wave packet generation method by superposing multiple plane waves, this study of ours presents an alternative approach towards obtaining a wave packet solution of a free particle relativistic Dirac equation. In this paper, we present Dirac’s free particle equation with a modification in the generalized momentum. The modification is achieved by coupling the momentum with a spatially varying logarithmic function, and this alteration does not affect the relativistic dispersion relation of the particle. Moreover, a solution of this modified Dirac equation is provided as well, which has been calculated using a trial wave function. The wave function solution is carried out in one dimension, where it behaves as a wave packet for a given ratio of the envelope parameter to the reduced Planck's constant greater than unity, where the envelope parameter regulates the width of the wave packet. The solution, being subject to this constraint, represents a bound particle with spin and a continuous energy spectrum.
Published in | International Journal of High Energy Physics (Volume 7, Issue 2) |
DOI | 10.11648/j.ijhep.20200702.11 |
Page(s) | 32-36 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
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Copyright © The Author(s), 2020. Published by Science Publishing Group |
Modified Dirac Equation, Localized Wave Packet, Generalized Momentum, Logarithmic Coupling
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APA Style
Mash-Huda Rahman Shipra, Syed Badiuzzaman Faruque. (2020). Investigation of an Equation with Logarithmic Coupling with Momentum in Dirac Equation. International Journal of High Energy Physics, 7(2), 32-36. https://doi.org/10.11648/j.ijhep.20200702.11
ACS Style
Mash-Huda Rahman Shipra; Syed Badiuzzaman Faruque. Investigation of an Equation with Logarithmic Coupling with Momentum in Dirac Equation. Int. J. High Energy Phys. 2020, 7(2), 32-36. doi: 10.11648/j.ijhep.20200702.11
AMA Style
Mash-Huda Rahman Shipra, Syed Badiuzzaman Faruque. Investigation of an Equation with Logarithmic Coupling with Momentum in Dirac Equation. Int J High Energy Phys. 2020;7(2):32-36. doi: 10.11648/j.ijhep.20200702.11
@article{10.11648/j.ijhep.20200702.11, author = {Mash-Huda Rahman Shipra and Syed Badiuzzaman Faruque}, title = {Investigation of an Equation with Logarithmic Coupling with Momentum in Dirac Equation}, journal = {International Journal of High Energy Physics}, volume = {7}, number = {2}, pages = {32-36}, doi = {10.11648/j.ijhep.20200702.11}, url = {https://doi.org/10.11648/j.ijhep.20200702.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijhep.20200702.11}, abstract = {The free particle solutions of the relativistic Dirac equation are characterized by plane waves with infinite uncertainty in position. However, many practical implementations of the solutions require a wave packet configuration, which can be utilized to represent a localized Dirac particle. Unlike the traditional wave packet generation method by superposing multiple plane waves, this study of ours presents an alternative approach towards obtaining a wave packet solution of a free particle relativistic Dirac equation. In this paper, we present Dirac’s free particle equation with a modification in the generalized momentum. The modification is achieved by coupling the momentum with a spatially varying logarithmic function, and this alteration does not affect the relativistic dispersion relation of the particle. Moreover, a solution of this modified Dirac equation is provided as well, which has been calculated using a trial wave function. The wave function solution is carried out in one dimension, where it behaves as a wave packet for a given ratio of the envelope parameter to the reduced Planck's constant greater than unity, where the envelope parameter regulates the width of the wave packet. The solution, being subject to this constraint, represents a bound particle with spin and a continuous energy spectrum.}, year = {2020} }
TY - JOUR T1 - Investigation of an Equation with Logarithmic Coupling with Momentum in Dirac Equation AU - Mash-Huda Rahman Shipra AU - Syed Badiuzzaman Faruque Y1 - 2020/08/10 PY - 2020 N1 - https://doi.org/10.11648/j.ijhep.20200702.11 DO - 10.11648/j.ijhep.20200702.11 T2 - International Journal of High Energy Physics JF - International Journal of High Energy Physics JO - International Journal of High Energy Physics SP - 32 EP - 36 PB - Science Publishing Group SN - 2376-7448 UR - https://doi.org/10.11648/j.ijhep.20200702.11 AB - The free particle solutions of the relativistic Dirac equation are characterized by plane waves with infinite uncertainty in position. However, many practical implementations of the solutions require a wave packet configuration, which can be utilized to represent a localized Dirac particle. Unlike the traditional wave packet generation method by superposing multiple plane waves, this study of ours presents an alternative approach towards obtaining a wave packet solution of a free particle relativistic Dirac equation. In this paper, we present Dirac’s free particle equation with a modification in the generalized momentum. The modification is achieved by coupling the momentum with a spatially varying logarithmic function, and this alteration does not affect the relativistic dispersion relation of the particle. Moreover, a solution of this modified Dirac equation is provided as well, which has been calculated using a trial wave function. The wave function solution is carried out in one dimension, where it behaves as a wave packet for a given ratio of the envelope parameter to the reduced Planck's constant greater than unity, where the envelope parameter regulates the width of the wave packet. The solution, being subject to this constraint, represents a bound particle with spin and a continuous energy spectrum. VL - 7 IS - 2 ER -