Understanding Spin States: Theoretical Minimum and Normal Coordinate Systems

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SUMMARY

The discussion clarifies that spin states for particles with spin 1/2 are represented by two eigenstates: "up" and "down." These states arise from the Dirac equation and are defined in a normal coordinate system where the z-direction is the reference for magnetic fields. All possible spin directions can be expressed as linear combinations of these two states, allowing for representation in any direction. This theoretical framework is applicable in practical scenarios such as neutron diffraction.

PREREQUISITES
  • Understanding of quantum mechanics, specifically spin-1/2 particles
  • Familiarity with the Dirac equation
  • Knowledge of eigenstates and their significance in quantum systems
  • Basic concepts of vector spaces and linear combinations
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  • Study the implications of the Dirac equation on particle spin states
  • Explore the application of spin states in neutron diffraction techniques
  • Learn about spherical polarimetry and its relevance in quantum mechanics
  • Investigate the mathematical representation of spin states in abstract vector spaces
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Physicists, quantum mechanics students, and researchers interested in the behavior of spin-1/2 particles and their applications in experimental physics.

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In The theoretical Minimum we shown all spins states use just two states up and down. How can we do that.?
I am confused about the directions of states and normal coordinate system Can somebody help me ?
Thanks
 
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Quarlep said:
In The theoretical Minimum
What does that mean?

If you measure the spin direction of a particle with spin 1/2, the only possible measurements are "up" and "down". If the particle has a different spin, the options are different.
Which normal coordinate system?
 
The spin value 1/2 and two spin states drop out of the Dirac equation. Spin-up and spin-down are chosen more or less arbitrarily, because they are the eigenstates of energy in a static magnetic field along the z-direction (theoretical magnetic fields are always along z...). However, they form a complete basis for spin-1/2 particles, and all spin directions can be written as a linear combination of these two basis states.

Therefore you can have spin directions in each and any direction. The theory is perfectly well developed and used e.g. in neutron diffraction.

https://www.ill.eu/en/instruments-support/instruments-groups/instruments/d3/how-it-works/spherical-polarimetry-with-cryopad/
 
Quarlep said:
In The theoretical Minimum we shown all spins states use just two states up and down. How can we do that.?

Think of spin-up as a vector pointing east and spin-down as a vector pointing north. We can write any vector as a linear combinations of those two. For example, north-east would be the vector sum of north and east, southeast would be their east minus north, and so forth.

The confusing thing is that the "directions" these vectors point in their abstract vector space isn't the same as the direction that the spin angular momentum vector points in the real world. Spin-up and spin-down are represented by orthogonal vectors in the abstract vector space, even though up and down are opposite directions.
 

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