The half-line square-root potential well is confining for , which is assumed here. The hard wall imposes and the smooth turning point is . With , the WKB action becomes
The hard-wall and soft-turning-point WKB quantization condition therefore gives
The coefficient here denotes the potential strength, not the integration limit in the generic quantization formula.
The WKB approximation is reliable in the interior where , but fails near the soft turning point where ; a connection formula supplies its phase. The hard wall also requires its boundary condition, and makes the local slow-variation condition fail sufficiently close to zero. Higher-energy states have a larger action relative to , with smaller relative endpoint regions, so the leading WKB spectrum is generally more reliable at large than for the ground state.
For , the exponential variational trial for a square-root half-line well satisfies the wall boundary condition and has norm . integration by parts has no boundary term and gives
The supplied gamma integral gives
Setting yields the unique minimum,
At the minimum , so the variational ground-state estimate is
The energy diverges as or , confirming that the stationary point minimizes the trial energy.
Write . Then and . The variational method guarantees , since the trial satisfies the wall condition and has finite energy. WKB gives no comparable upper-bound guarantee and is least controlled for the lowest state. The two estimates differ by about of the WKB value; their closeness is encouraging but does not prove that the exact energy lies between them.

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