Geometric Algebra formulation of Quantum Mechanics

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Discussion Overview

The discussion revolves around the application of Geometric Algebra (GA) to Quantum Mechanics (QM), specifically focusing on the mapping between normalized spinors and rotors as described in "Geometric Algebra for Physicists." Participants seek clarification on mathematical definitions and the implications of this mapping in the context of quantum theory.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant expresses interest in deriving the mapping between normalized spinors and rotors and seeks guidance on this process.
  • Another participant notes that proving a one-to-one mapping is essential and discusses the relationship between the components of the mapping and the Pauli operators.
  • Several participants express uncertainty about the meaning of "map" in this context and the significance of the variable "a" and its superscripts.
  • One participant suggests that the mapping is crucial for demonstrating that GA can yield results similar to those obtained using specialized Pauli operators.
  • Another participant attempts to connect the concept of the Pauli matrices forming a Clifford algebra to the representation of spinor wavefunctions as rotors, emphasizing the geometric insights this may provide.

Areas of Agreement / Disagreement

Participants generally agree on the importance of the mapping in understanding the relationship between GA and QM, but there is no consensus on the precise mathematical definitions or implications of the variables involved. Multiple views on the interpretation of the mapping and its components remain unresolved.

Contextual Notes

Participants express uncertainty about specific mathematical definitions and the roles of certain variables in the mapping, indicating that further clarification is needed to fully understand the concepts discussed.

Milsomonk
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Hi all,
I'm reading a paragraph from "Geometric Algebra for Physicists" - Chris Doran, Anthony Lasenby. I'm quite interested in applying GA to QM but I've got to a stage where I am not following part of the chapter and am wondering if someone can shed a little light for me.
upload_2016-12-19_12-15-53.png

The part I'm not quite sure about is the bit at the bottom where a "map" is found between the normalised spinor and the rotor. I guess I'm just not sure how I might derive this myself, which I would like to do, as I have done for the rest so far. Any guidance would be much appreciated, and wishing all a happy festive season :)
 
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The only thing to prove is that there is a mapping that is 1-1. The right side of 8.20 expands to
a0 + a1Iσ1+ a2Iσ2+ a3Iσ3
Since the match-ups of the ai on the left and right side are obvious, the 1-1 mapping follows.
The motivation of why he would want to match the two sides up that way, (with sign changes, etc.), is that the calculations of the right side are very methodically defined in geometric algebra and can be used in many situations. The GA calculations and definitions are not specific to this application, whereas the left side Pauli operators have to be specifically defined for that application.
 
Hi, Thanks very much for your reply, it deffinately helps :) I guess I'm not really sure what map means in this context, I sort of have a vague idea but am lacking a more mathematical definition. I'm not really sure what a represents and it's superscript numbers.
 
Milsomonk said:
Hi, Thanks very much for your reply, it deffinately helps :) I guess I'm not really sure what map means in this context, I sort of have a vague idea but am lacking a more mathematical definition. I'm not really sure what a represents and it's superscript numbers.
The mapping means very little on its own. The book should show that one can do routine GA calculations and get back to the same results that required specialized Pauli operators. Once that is accomplished, you should see if GA offers some routine, methodical, insight into the physical results that were less obvious without GA.
 
Yeah basically what I'm trying to do is show that you can use the fact that the pauli matrices form a clifford algebra of space, to write the spinor wavefunction as a rotor, thus lending a little more geometric insight into the link between complex numbers and spin. This map appears to be an important component but I simply don't understand what "a" represents.
 
Milsomonk said:
Yeah basically what I'm trying to do is show that you can use the fact that the pauli matrices form a clifford algebra of space, to write the spinor wavefunction as a rotor, thus lending a little more geometric insight into the link between complex numbers and spin. This map appears to be an important component but I simply don't understand what "a" represents.
It looks to me like the ais come from the real and imaginary parts of equation 8.16. Beyond that, I can't help you because I don't really know anything about that physics subject.
 
Hmm, yeah I wondered that. Thanks for your help :)
 

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