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The connection to twistor theory is I think not hard to see. The boost operator P_μ that acts on [x_i, x_0] = ilx_i such that
P_μ > [x_i, x_0] = il P_μ > x_i
The coordinates (x_j, x_0) we write in spinor form
x_j = σ_j^{aa'}ω_{aa'}
x_0 = σ_0^{aa'}ω_{aa'},
where ω_{aa'} = ξ_a ω_{a'} ξ_{a'}ω_a. This commutator has the form
[x_i, x_0] = σ_j^{aa'}σ_0^{bb'}[ω_{aa'}, ω_{bb'}]
= iC^{cc'}_{aa'bb'} σ_j^{aa'} σ_0^{bb'} ω_{aa'}
= i|C| σ_j^{aa'}ω_{aa'}
where the magnitude of the structure matrix is |C| = l. In general this may be written for
x_j = σ_j^{aa'}ω_{aa'}
x_0 = σ_0^{aa'}ω_{aa'} iq_{aa'}π^{aa'},
where the commutator [ω_{aa'}, π^{bb'}] = iδ_a^bδ_{a'}^{b'} and the general form of the commutator is then
[x_i, x_0] = i|C| σ_j^{aa'}ω_{aa'} iσ_j^{aa'}q_{bb'}[ω_{aa'}, π^{bb''}
[x_i, x_0] = ilσ_j^{aa'}ω_{aa'} - σ_j^{aa'}q_{aa'}.
The boost operation B = 1 a^l_jP^j on the commutator [x_i, x_0] is then equivalent to the commutation between spinors [ω_a, ω'_b] for ω'_b = ω_b iq_{bb'}π^{b'},
[ω_a, ω'_b] = [ω_a, ω_b] iq_{bb'}[ω_a , π^{b'}]
= C^c_{ab} ω_c iq_{ab}.
This could be explored more deeply. Ed Witten demonstrated the "twistor revolution" in string theory. If twistors are connected to κ-Minkowski spacetime there might then be a link between string theory and LQG and other "edgelink" type of quantum gravity theories. This would be potentially interesting, for this might serve to correct the difficulties with each of these.
Cheers LC