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Collaborators and some publications Introduction Action <strong>of</strong> the <strong>Approach</strong> Yukawa couplings and scalar fields <strong>The</strong> spinor represent<br />

A simple action for a spinor which carries in d = (1 + 13) only<br />

two kinds <strong>of</strong> a spin (no charges) and for the gauge fields<br />

∫<br />

S = d d x E L f +<br />

∫<br />

d d x E (α R + ˜α ˜R),<br />

L f = 1 2 (E ¯ψ γ a p 0a ψ) + h.c.<br />

p 0a = f α ap 0α ,<br />

p 0α = p α<br />

− 1 2 Sab ω abα − 1 2 ˜S ab˜ω abα<br />

N.S. Mankoč Borštnik, Cape Town 2010, 01-06 February University <strong>of</strong> Ljubljana<br />

<strong>The</strong> <strong>Approach</strong> Unifying spins and charges

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