Understanding Spin & Angular Momentum in Quantum Mechanics

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SUMMARY

The discussion clarifies that in quantum mechanics, the spin-singlet state of two particles, represented as $$|S=0,M=0 \rangle=\frac{1}{\sqrt{2}} (|1/2,-1/2 \rangle-|1/2,+1/2 \rangle)$$, ensures that measuring the spin of one particle in any direction guarantees that the spin of the second particle will yield the opposite result. This property holds true regardless of the axis chosen for measurement, as the total spin of the system is zero, making it invariant under rotations. Thus, the description of spin does not limit itself to the z-axis.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically spin and angular momentum.
  • Familiarity with quantum states and notation, such as singlet states and basis transformations.
  • Knowledge of rotation invariance in quantum systems.
  • Basic mathematical skills to interpret quantum state representations.
NEXT STEPS
  • Study the implications of spin and angular momentum in quantum mechanics.
  • Learn about the mathematical representation of quantum states and basis transformations.
  • Explore the concept of rotation invariance and its effects on quantum systems.
  • Investigate the measurement theory in quantum mechanics, focusing on entangled states.
USEFUL FOR

Students and professionals in physics, particularly those specializing in quantum mechanics, quantum computing, and theoretical physics, will benefit from this discussion.

Silviu
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Hello! I got a bit confused about the fact that the whole the description of spin (and angular momentum) is done in the z direction. So, if we are told that a system of 2 particles is in a singlet state i.e. $$\frac{\uparrow \downarrow -\downarrow \uparrow }{2}$$ does this mean that measuring the spin of the first one on ##\textbf{any}## axis (not only z) will ensure that measuring the spin of the second one will give the opposite result? Or is this form true only for the z axis, and if we want to check on other axis, we need to project the up and down of the z axis onto the orthonormal basis of this other system of axis and work from there? Thank you!
 
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The correctly normalized singlet state is
$$|S=0,M=0 \rangle=\frac{1}{\sqrt{2}} (|1/2,-1/2 \rangle-|1/2,+1/2 \rangle).$$
It's true that if measuring the spin component in an arbitrary direction of particle 1 then the spin component of particle 2 in the same direction is opposite. It doesn't matter which basis you use to describe the spin-singlet state. The reason is that for total spin ##S=0## the state doesn't change under rotations, i.e., you cannot distinguish any spin direction from any other.
 

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