Let the common on-site energy be zero and the common hopping magnitude be t=∣β∣. Consistent with the axial-p convention and the formula in part (iii), the hopping signs are βs=−t and βp=+t.
The curves cross at k=π/(2a), E=0, with no gap. The lower-left panel shows the continuous pure-s and pure-p branches. Their identities remain fixed through the crossing; the energy-ordered lower state changes from s to p character on passing through it.