Pauli.m

Pauli matrices (sparse, see below for normalisation conventions) for a spin of a user-specified energy level multiplicity.

Syntax

    S=pauli(mult)

Parameters

    mult - an integer specifying the 
           multiplicity of the spin

Outputs

    S.u - unit operator

    S.p - raising operator

    S.m - lowering operator

    S.x - Sx observable operator

    S.y - Sy observable operator

    S.z - Sz observable operator

Notes

1. The matrices are normalized so as to obey the following commutation relations:

         [S.x,S.y]=1i*S.z
         [S.y,S.z]=1i*S.x
         [S.z,S.x]=1i*S.y

2. Raising and lowering operators are defined as:

          S.p=S.x+1i*S.y
          S.m=S.x-1i*S.y

3. It is never a good idea to normalise spin operators using matrix norms because commutation relations would break.

4. The arrays are declared complex at creation to avoid expensive reallocations later on.

See also

stevens.m, irr_sph_ten.m, wigner.m, operator.m, state.m, hamiltonian.m, add_spins.m, cg_fast.m, clebsch_gordan.m, comm.m, hilb2liouv.m, ist_product_table.m, lorentz.m, mat2sphten.m, multipack.m, perm_group.m, rocomm.m, rwalk.m, sle_operators.m, sorensen.m, spher_harmon.m, sphten2mat.m, stev2sph.m, superop.m, twospinist.m, wigner_3j.m, wigner_6j.m, Kernel_utilities

Version 2.8, authors: Ilya Kuprov