Spinors, vectors and quaternions

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SUMMARY

Spinors and vectors are distinct mathematical entities, where spinors represent SU(2) and vectors represent SO(3). Both can be expressed using quaternions, with vectors defined as Vq = ix + jy + kz and spinors as Sq = ix + jy + kz. The Pauli matrices, specifically σ_x, σ_y, and σ_z, play a crucial role in the representation of these entities, with spinors being 2-component complex vectors. The basis for the Clifford algebra in this context includes σ_0, σ_x, σ_y, σ_z, and their imaginary counterparts.

PREREQUISITES
  • Understanding of SU(2) and SO(3) groups
  • Familiarity with Pauli matrices
  • Knowledge of quaternions
  • Basic concepts of Clifford algebra
NEXT STEPS
  • Research the mathematical properties of SU(2) and SO(3)
  • Study the applications of Pauli matrices in quantum mechanics
  • Explore quaternion algebra and its uses in physics
  • Learn about Clifford algebra and its significance in geometry
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Mathematicians, physicists, and computer scientists interested in advanced algebraic structures, particularly those working with quantum mechanics and geometric interpretations of spinors and vectors.

dimsun
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I am interested in using hypercomplex numbers and not using tensors.

Therefore a question about the difference between spinors and vectors.
I read that they both can be written as quaternions.

Vector:
Vq = ix + jy + kz

Spinor:
Sq = ix + jy + kz

So what is the difference between them?
Can anyone tell me?

Dimsun
 
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Can you give some references or link where you read this, for the people who are not so familiar with this stuff but would like to help? :)

I'm not into quaternions, but the short answer to your question is that spinors are representations of SU(2) and vectors are representations of SO(3), where SU(2) is the double cover of SO(3).
 
I think it goes something like this. If \sigma_x , \sigma_y , \sigma_z are the Pauli matrices, then \sigma_0 , i\sigma_x , i\sigma_y , i\sigma_z act like the unit quaternions, where \sigma_0 is the 2x2 identity matrix and i=\sqrt{-1}. A vector v can be written v = v_x\sigma_x + v_y\sigma_y + v_z\sigma_z and a spinor can be written \psi = \alpha\sigma_0 + \beta i\sigma_x + \gamma i\sigma_y + \delta i\sigma_z where \alpha, \beta, \gamma, \delta are all real. You get back to the idea of spinors as 2-component complex vectors by writing
|\psi\rangle = \left(\begin{array}{c}<br /> \alpha +i\delta \\<br /> -\gamma + i\beta\end{array}\right)

The set \sigma_0 , \sigma_x , \sigma_y , \sigma_z , i\sigma_x , i\sigma_y , i\sigma_z , i\sigma_0 forms a basis for the Clifford algebra.

This is in 3-d, no idea about 4-d.

At least I think some of that is right...
 

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