. Barton, Elements of Green's Functions and Propagation Clarendon Press, 1989.

P. Feynman and A. R. Hibbs, Quantum Mechanics and Path Integrals McGraw-Hill, 1965.

I. E. Abramowitz and . Stegun, Handbook of Mathematical Functions Dover, 2000.

D. Landau and E. M. Lifchitz, The Classical Theory of Fields 52 The stationary phase method could also provide a way to calculate this integral, 1975.

J. Riou, Institut d'Optique 60 A detailed development of the first term of Eq. 11 using the stationary phase approximation leads to the value B = R / i / 2 59. However, in practice, as long as one is interested only in the shape of the wave function, the precise value of C is not necessary, 2006.

=. ?-since-the-normalization, A. , and R. , A more accurate treatment is thus needed to deal with the few trajectories starting at the edge of the rf knife. One possibility is to use the exact solution of the radially symmetric twodimensional inverted potential, as presented in Eq

A. Fertig and B. I. Halperin, Transmission coefficient of an electron through a saddle-point potential in a magnetic field, Physical Review B, vol.36, issue.15, p.7969, 1987.
DOI : 10.1103/PhysRevB.36.7969