Dirac equation and clifford algebra

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SUMMARY

Understanding the derivation of the Dirac equation does not strictly require knowledge of Clifford algebra, although it naturally emerges during the process. The discussion highlights that many introductory texts utilize a linear Hamiltonian operator to reproduce the relativistic energy-momentum-mass relationship, leading to the realization of Clifford algebra through Dirac matrices. Sources such as the arXiv paper and Sommerfeld's "Atombau und Spektrallinien" provide alternative derivations that do not explicitly use Clifford algebra. Ultimately, regardless of the method, the Dirac formalism is a natural representation of the Lorentz group, essential for describing parity-conserving interactions.

PREREQUISITES
  • Familiarity with the Dirac equation and its significance in quantum mechanics.
  • Understanding of linear Hamiltonian operators in quantum physics.
  • Basic knowledge of relativistic energy-momentum-mass relationships.
  • Awareness of Dirac matrices and their role in quantum field theory.
NEXT STEPS
  • Research "Dirac matrices and their representations" to understand their application in quantum mechanics.
  • Study the derivation of the Dirac equation using linear Hamiltonian operators.
  • Explore alternative mathematical frameworks such as quaternions in the context of quantum mechanics.
  • Examine the arXiv paper referenced for insights into deriving the Dirac equation without Clifford algebra.
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Physicists, mathematicians, and students interested in quantum mechanics, particularly those exploring the foundations of the Dirac equation and its derivations.

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Is it a must to know clifford algebra in order to derive the dirac equation?
I recently watch drphysics video on deriving dirac equation and he use two waves moving in opposite directions to derive it, without touching clifford algebra. If this possible, what is the intuition behind it?
 
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No you don't "need to" know Clifford Algebra... you derive it in the process in order to get your equation working [and reproducing the relativistic relationship between energy and mass/momenta] . At least by the time one adds the gamma matrices..
 
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ChrisVer said:
No you don't "need to" know Clifford Algebra... you derive it in the process in order to get your equation working [and reproducing the relativistic relationship between energy and mass/momenta] . At least by the time one adds the gamma matrices..
Do you have any sources that will allow me to derive the dirac equation without clifford algebra? Cause I have been searching on the Internet and all of it involves clifford algebra. Besides the one by drphysics he didnt really derive it fully such as the dirac matrix.
 
I haven't seen what you are talking about, I don't know which is that drphysics book... Maybe this can help? http://arxiv.org/vc/quant-ph/papers/0607/0607001v1.pdf (sec.4)

However, I don't understand this "clifford algebra" thing. In every introductory book, they never used the Clifford algebra to derive the Dirac equation.
Most of them are starting by a linear Hamiltonian operator, which they act to reproduce the result of the relativistic energy-momentum-mass relation E^2 = m^2 +p^2. By doing so, you see that the objects that you used in your operator were not just complex numbers, but they should satisfy certain relations, one of them is the Clifford Algebra. You don't "use" it, you "result" in it...
 
Well, you can call it as you like. The Clifford algebra is basically the algebra realized in the usual treatment by the Dirac matrices in the one or the other representation. At some time ago in history also quaternions and octonions were en vogue. In the 19th century at least; Maxwell formulated his equations first in terms of quaternions; the usual vector notation was introduced into physics by Heaviside and became widely used in the beginning of the 20th century. It was not the least spread by the famous Handbook "Enzykloädie der mathematischen Wissenschaften", edited by Felix Klein around 1900. You can find a derivation of the Dirac equation, using quaternions in the even more famous book by Sommerfeld "Atombau und Spektrallinien" (freely translated: Atomic Structure and Spectral Lines). As stressed before: No matter, how you derive it you end up with somehow with the Dirac formalism. This is no surprise, because it's a very natural representation of the proper orthochronous Lorentz group augmented by spatial reflections to be able to describe the parity-conserving interactions, especially the electromagnetic interaction, which was the first application of the Dirac formalism of course.
 

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