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The opposite spatial parity of the s orbital and axial p orbital gives opposite signs for left and right $s$–$p$ hopping. With real ${\beta }_{sp}$, one consistent Bloch-basis convention givesThe resulting energies areThus s-p mixing in a one-dimensional tight-binding chain lowers the lower branch and raises the upper branch wherever the coupling is nonzero. For separated atomic levels, the lower branch remains mainly $s$ and the upper mainly $p$, with increasing admixture where their uncoupled energies approach.

The upper-right panel of the figure in part (a)(ii) compares the mixed curves with dashed unmixed curves. The mixing vanishes at both $k=0$ and $\pi /a$, so those endpoints remain unchanged. If the unmixed curves approach or cross in the interior, the nonzero coupling produces an avoided crossing.