To construct a self-adjoint operator the domain of the operator has to be specified by imposing an appropriate boundary condition or conditions on the wave functions on which the operator acts. We illustrate situations for which different boundary conditions lead to different operators and hence to different physics.

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We call this domain C0((0,∞)\{0}). The symbol C means that the functions are continuous. The superscript ∞ means that the functions are infinitely differentiable. The subscript 0, and the removal of the origin, \{0}, means that all the functions in the domain vanish in a small, but finite interval [0,a] where a>0 is an arbitrary real number, and also for x>b>a, another arbitrary real number.
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We call this domain C0(R\{0}). The meaning of the symbol R\{0} is that the point zero has been removed from the real line. So the functions in this domain are not defined for x=0. The superscript ∞ and the subscript 0 have the same meanings as before; \{0}, means that the functions uabcd(x) belonging to C0(R\{0}) vanish around x=0, that is for −a<x<b and also for x<−c and for x>d, where a,b,c, and d are arbitrary positive numbers. Therefore the domain of this operator consists of functions that vanish before the point x=0 from the negative and positive sides and for large distances in both positive and negative directions.
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In the mathematical literature the two equations (A5) and (A6) are written with O replaced by O+. In this way we don’t need to say anything about the domain.
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