next up previous
Next: Addition of Angular Momenta Up: Spin Angular Momentum Previous: Spin Angular Momentum

Spinors

In the basis tex2html_wrap_inline6023 , a general spin state tex2html_wrap_inline6171 can be written as

equation3521

with complex coefficients tex2html_wrap_inline6173 . Normalisation requires that

equation3529

The state tex2html_wrap_inline6171 defined above can also be represented by a two-component column vector called a spinor whose components are given by the projections onto the basis tex2html_wrap_inline6023 :

eqnarray3537

The basis spinors are

eqnarray3545

and the completeness relation in this matrix representation is

equation3547

truein


truein Problem :19 An electron is in the spin state

displaymath6179

truein


truein

Spin is an additional degree of freedom independent of the spatial degrees of freedom. Spin and position (or momentum) can assume precise values simultaneously and independently of one another i.e.

equation3567

equation3569

equation3571

The total quantum state of a particle is constructed from the direct product of the position and spin eigenstates. The states tex2html_wrap_inline6191 and tex2html_wrap_inline6193 forms a basis for the Hilbert space (that takes into account the spatial and spin degrees of freedom). A general state tex2html_wrap_inline6195 in this Hilbert space is then given by

equation3585

The projection onto position and spin eigenstates are

eqnarray3602

since tex2html_wrap_inline6197 and

eqnarray3634

The quantities tex2html_wrap_inline6199 express the probability of finding the particle at position tex2html_wrap_inline6201 with z-component of spin of tex2html_wrap_inline5991 . The normalisation condition is

eqnarray3668



Gunaretnam Rajagopal
Tue Oct 15 17:55:22 BST 1996