With phase , the original ray is a contour integral. At the endpoint , the steepest direction solves with decreasing real part; locally it is the direction for which is negative real.
The saddle is . Completing the square gives , so its steepest-descent line is the horizontal line , .
Deform the real ray upward to the saddle line, joining it near the endpoint and at a large right cutoff. The integrand is entire. The far bridge vanishes by Gaussian decay; the endpoint bridge is because .
The saddle contributes the full Gaussian
Thus . Since the phase is exactly quadratic, there are no further algebraic saddle terms; the next contribution is the endpoint term .

Articles by others on the same topic (0)

There are currently no matching articles.