“…[1] For the W-sector, the effective potential Vw = V st w + V o w , where the first term is the statistical part and the second one is the Euler-Heisenberg vacuum term. We can consider Vw ≈ V st w (see [7]). [2] We write ξ 2 where i = 1, 2; κ i = 5, 1 respectively, and 0 ≤ x 1 ≤ 1/ √ 3, 1/ √ 3 ≤ x 2 ≤ 1.. Due to the fact that E is proportional to N w , we deduce that for each N w , there are two possible values of the symmetry breaking parameter y 1,2 .…”