Calculating Helicity in Non-Relativistic Quantum Mechanics using Pauli Matrices

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SUMMARY

The helicity in non-relativistic quantum mechanics is defined by the equation ##\sigma \cdot p / |p|##, where ##\sigma## represents the Pauli matrices and ##p## denotes momentum. In spinor space, the Pauli matrices are 2x2 matrices, leading to a helicity that is a 2x2 quantity. However, in three-dimensional physical space, the helicity is expressed as an inner product of three-vectors, resulting in a 1x1 quantity. The scalar helicities ##\pm\frac{1}{2}\hbar## are eigenstates of the helicity operator, but general states with misaligned spin and momentum do not yield eigenstates.

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Tio Barnabe
The helicity in non relativistic quantum mechanics is given by ##\sigma \cdot p / |p|## where ##\sigma## are the pauli matrices and ##p## the momentum. In spinor space, the ##\sigma## are 2x2 matrices, and thus, the helicity, if we calculate it, is a 2x2 quantity. But in 3d physical space, the above equation is an inner product between two three-vectors, because we have three pauli matrices. It's like ##\sigma_i p^i## and thus the helicity is a 1x1 quantity.

My question is, How can I transform the pauli matrices, such that each matrix ##\sigma_i## becomes a number, such that I get the latter result I mentioned above? Maybe taking their determinant?
 
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Tio Barnabe said:
The helicity in non relativistic quantum mechanics is given by ##\sigma \cdot p / |p|## where ##\sigma## are the pauli matrices and ##p## the momentum. In spinor space, the ##\sigma## are 2x2 matrices, and thus, the helicity, if we calculate it, is a 2x2 quantity. But in 3d physical space, the above equation is an inner product between two three-vectors, because we have three pauli matrices. It's like ##\sigma_i p^i## and thus the helicity is a 1x1 quantity.

My question is, How can I transform the pauli matrices, such that each matrix ##\sigma_i## becomes a number, such that I get the latter result I mentioned above? Maybe taking their determinant?

The Pauli matrices and the corresponding helicity operator ##\sigma \cdot p / |p|## are operators, not scalars. The scalar helicities ##\pm\frac{1}{2}\hbar## are eigenstates of the helicity operator.
 
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mikeyork said:
The scalar helicities ##\pm\frac{1}{2}\hbar## are eigenstates of the helicity operator.
what if we have a general state with spin and momentum not aligned. In this case it will not be an eigenstate of the helicity operator.
 
Tio Barnabe said:
what if we have a general state with spin and momentum not aligned. In this case it will not be an eigenstate of the helicity operator.
That's right. It will be a superposition -- or a spin eigenstate along another axis.
 
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