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HomogenousCow
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I'm currently reading the Griffith book and he dosen't really explain this, do i just miltiply the spin kets with the wave function??
andrien said:In non relativistic quantum mechanics spin is introduced in a rather ad hoc manner and by solving the schrodinger 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 schrodinger 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.
The spin of a particle, such as an electron, is an intrinsic quantum property that affects its behavior in a magnetic field. This spin must be incorporated into the wavefunction in order to accurately describe the particle's properties and interactions.
Yes, spin can be incorporated into any wavefunction, as long as the wavefunction is expressed in terms of the correct basis set. For example, when dealing with spin-1/2 particles, the wavefunction must be expressed in terms of two basis states, corresponding to the two possible spin orientations.
The mathematical representation of spin in the wavefunction is through the use of spin operators. These operators act on the wavefunction to extract information about the particle's spin, such as its magnitude and orientation.
The inclusion of spin can result in a change in the wavefunction's symmetry. For example, in a system with two identical particles, the wavefunction must be anti-symmetric when the particles have half-integer spin, and symmetric when the particles have integer spin.
Yes, incorporating spin into the wavefunction is essential for accurately describing and predicting the behavior of particles in various systems, such as atoms, molecules, and solid materials. It is also crucial for understanding phenomena such as magnetism and superconductivity.