The Approach of
The Approach of
The Approach of
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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 />
In the S ab sector appear massless gauge fields <strong>of</strong><br />
Y = τ 4 + τ 23 , and τ 1i ,<br />
˜τ 1 = ( 1 2 (S 58 − S 67 ), 1 2 (S 57 + S 68 ), 1 2 (S 56 − S 78 ))<br />
and massive <strong>of</strong> τ 2i ,<br />
˜τ 2 = ( 1 2 (S 58 + S 67 ), 1 2 (S 57 − S 68 ), 1 2 (S 56 + S 78 ))<br />
Similar breaks occur in the ˜S ab sector.<br />
<strong>The</strong> properties <strong>of</strong> the upper massive four families are under<br />
consideration, treating loop corrections.<br />
<strong>The</strong> lowest one <strong>of</strong> the upper four families (all with no<br />
Yukawa couplings to the lowest four families) is<br />
predicted to constitute the dark matter.<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