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 becomesThe hard-wall and soft-turning-point WKB quantization condition therefore givesThe 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 givesThe supplied gamma integral givesSetting yields the unique minimum,At the minimum , so the variational ground-state estimate isThe 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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