Factorizing the projector found in part b gives the normalized eigenfunctionswith zero continuation outside. Their squared integrals are one and different positive integers give orthogonal functions. These are the familiar infinite-square-well states shifted so that the well centre is at zero. Each eigenfunction has an arbitrary overall constant phase, which cancels from the projector.
φn(x)=a2sinanπ(x+a/2),−a/2<x<a/2,n≥1,
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