By the evenness of , the semiclassical action integral is twice its integral over the positive half-axis. If , then
If , split the integral at :
The first integral is
In the second, put and then . It becomes
After simplification,
This is the action integral for a linear-to-square-root potential.
The graph begins at the origin, is continuous and strictly increasing, passes through , and tends to infinity. Therefore for every and , the equation
has exactly one solution by the intermediate value theorem and strict monotonicity.

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