\prob{52}
A particle of mass m is confined to an infinitely deep squarewell potential:
The normalized eigenfunctions, labeled by the quantum number n, are
The eigenfunctions satisfy the condition if , otherwise . This is a statement that the eigenfunctions are
 solutions to the Schrodinger equation
 orthonormal
 bounded
 linearly dependent
 symmetric

Quantum Mechanics}Orthonormality
This is the definition of orthonormality, i.e., something that is both orthogonal (self dot others = 0) and normal (self dot self = 1).
