WriteThe saddle equation is unchanged, soThe contour connected to the original positive-real integration path passes through . Since , its steepest-descent branch hasFor and ,Thus the contour equation isIt approaches the origin along the positive imaginary axis, passes through , , and tends to infinity along the positive real axis. Along both ends the real part of the phase tends to , so the contour rises from the origin nearly vertically, bends through the first-quadrant saddle, and leaves nearly horizontally. The other saddle lies on a different constant-imaginary-phase contour and does not connect to this deformation.
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