HomogenousCow
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I'm currently reading the Griffith book and he doesn't really explain this, do i just miltiply the spin kets with the wave function??
This discussion centers on the incorporation of spin into wavefunctions in quantum mechanics, specifically addressing the methodologies outlined in Griffith's textbook. Participants clarify that spin degrees of freedom do not interfere with coordinate degrees of freedom, leading to the multiplication of spin kets with wavefunctions dependent on spatial coordinates. The conversation highlights historical perspectives on spin, contrasting the ad hoc introduction in non-relativistic quantum mechanics with the logical derivation from Galilean and relativistic theories, referencing key works by Pauli and Lévy-Leblond.
PREREQUISITESQuantum physicists, students of quantum mechanics, and researchers interested in the theoretical foundations of spin and wavefunctions will benefit from this discussion.
andrien said:In non relativistic quantum mechanics spin is introduced in a rather ad hoc manner and by solving the Schrödinger eqn for say hydrogen atom one can introduce all quantum numbers but spin.Spin was introduced as another degree of freedom because it can not be obtained from Schrödinger eqn.However pauli introduced it for spin 1/2 by noting that p2 can be written as (σ.p)(σ.p),but it is still artificial.The logical way of introducing it was done by dirac for spin 1/2.
andrien said:I was saying it in historical way,nevertheless the reference you have given accepts the dirac original view to make a non-relativistic version of dirac eqn and it is not a logical consequence of Galilean theory because it nevertheless assumes linearity in both time and space derivative which was the original point of dirac in his paper.So i will still call it some way of fixing it,rather than some original motivation on Galilean relativity.