Multiplication between vector and vector operator

LagrangeEuler
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How this is defined?

##\vec{r}\cdot \vec{\sigma}##?
where ##\vec{r}=(x,y,z)## and ##\vec{\sigma}=(\sigma_x,\sigma_y,\sigma_z)##. ##\sigma_i## are Pauli spin matrices.
 
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It's a 2x2 matrix... It seems you've stumbled on the way to represent the location of a point in space as a 2x2 matrix instead of a vector. I'm fuzzy on the rigorous details, but it has something to do with the relationship between SO(3) and SU(2).
 
In quantum mechanics, both of those objects are operators. The operator \mathbf{r} operates on state vectors in real space, whereas the operator \sigma operates on spinors in spin space. You can treat (symbolically) the dot product between \mathbf{r} and \sigma as a normal dot product between two vectors, i.e.

\mathbf{r}\cdot\sigma=x\sigma_x+y\sigma_y+z\sigma_z

where the x,y,z,\sigma_x,\sigma_y,\sigma_z are all operators. Say we have a state |\psi\rangle=|\phi\rangle\otimes|\chi\rangle where |\phi\rangle is a state vector in real space and |\chi\rangle is a spinor. Then

\mathbf{r}\cdot\sigma|\psi\rangle=x\sigma_x|\psi\rangle+y\sigma_y|\psi \rangle+z\sigma_z|\psi\rangle
=x|\phi\rangle\otimes\sigma_x|\chi\rangle+y|\phi\rangle\otimes \sigma_y|\chi\rangle+z|\phi\rangle\otimes\sigma_z|\chi\rangle

where the operators x,y,z operate on the real space state vector |\phi\rangle and the operators \sigma_x,\sigma_y,\sigma_z operate on the spinor |\chi\rangle.
 
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