Does Quantum Contextuality only apply to spin?

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SUMMARY

Quantum contextuality applies not only to measurements of spin but also to momentum and position. The concept of spin arises from the need to account for an additional degree of freedom in quantum mechanics, which is not derived directly from the Schrödinger equation. Instead, spin must be included in the Hamiltonian of the system to manifest in quantum calculations. The mathematical formalism of quantum mechanics is inherently contextual, with spin and photon polarization being common examples due to their experimental accessibility.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly quantum contextuality.
  • Familiarity with the Schrödinger equation and its applications.
  • Knowledge of angular momentum in quantum systems.
  • Basic grasp of group theory as it relates to quantum physics.
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  • Study the implications of quantum contextuality in various quantum systems.
  • Explore the derivation of spin in quantum mechanics through Pauli's equation.
  • Investigate the role of group theory in quantum mechanics, focusing on the Galilei and Poincaré groups.
  • Examine experimental setups that demonstrate quantum contextuality using spin and photon polarization.
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Students and researchers in quantum physics, physicists exploring quantum mechanics, and anyone interested in the foundational aspects of quantum contextuality and spin.

Jarrodmccarthy
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I have just recently started learning about quantum contextuality and can only seem to find examples where contextuality is need to explain measurements of spin.
So I am curious as to whether quantum contextuality only applies to measurements of spin?

Also, If someone could clarify where the quantum number for spin 'comes from' since I haven't been able to find a solution where it comes out of the Schroedinger equation?

Any responses would be fantastic and apologies if the questions aren't well formulated.
 
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Jarrodmccarthy said:
Also, If someone could clarify where the quantum number for spin 'comes from' since I haven't been able to find a solution where it comes out of the Schroedinger equation?
Spin was discovered by observation. During the 1920s it became clear that a bound electron had an additional degree of freedom beyond the n,l,m quantum numbers that appear when you solve Schrödinger's equation for a spinless charged particle around the nucleus.

As with any observable, to make spin show up in Schrödinger's equation, you have to include it in the Hamiltonian. If the physical system is such that spin-related effects are negligible or non-existent (for example, a free electron in the absence of a magnetic field) then there won't be any spin-related terms in the Hamiltonian.
 
Jarrodmccarthy said:
I have just recently started learning about quantum contextuality and can only seem to find examples where contextuality is need to explain measurements of spin.
So I am curious as to whether quantum contextuality only applies to measurements of spin?
As far as the mathematical formalism of QM is concerned, everything is contextual. Spin and photon polarization are used as examples most often because it's relatively easy to design experiments using them to demonstrate contextually.
 
Nugatory said:
As far as the mathematical formalism of QM is concerned, everything is contextual. Spin and photon polarization are used as examples most often because it's relatively easy to design experiments using them to demonstrate contextually.
Thank you very much.
All of what you said made sense so thank you.
 
Quantum spin angular momentum is a consequence of group theory (Galilei group for Newtonian spacetime, Poincare group for Minkowski spacetime), and Pauli's equation for the non specially relativistic case follows as the only option to have a 2nd order PDE which incorporates spin. This derivation was made by Levy-Leblond in the golden era of the 1960's.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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