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36 Integrals with Coalescing SaddlesProperties

§36.9 Integral Identities

36.9.1 |Ψ1⁡(x)|2 =25/3⁢∫0∞Ψ1⁡(22/3⁢(3⁢u2+x))⁢du;
equivalently,
36.9.2 (Ai⁡(x))2 =22/3π⁢∫0∞Ai⁡(22/3⁢(u2+x))⁢du.
36.9.3 |Ψ1⁡(x)|2 =8⁢π3⁢∫0∞u−1/2⁢cos⁡(2⁢u⁢(x+u2)+14⁢π)⁢du.
36.9.4 |Ψ2⁡(x,y)|2 =∫0∞(Ψ1⁡(4⁢u3+2⁢u⁢y+xu1/3)+Ψ1⁡(4⁢u3+2⁢u⁢y−xu1/3))⁢duu1/3.
36.9.5 |Ψ2⁡(x,y)|2 =2⁢∫0∞cos⁡(2⁢x⁢u)⁢Ψ1⁡(2⁢u2/3⁢(y+2⁢u2))⁢duu1/3.
36.9.6 |Ψ3⁡(x,y,z)|2 =24/5⁢∫−∞∞Ψ3⁡(24/5⁢(x+2⁢u⁢y+3⁢u2⁢z+5⁢u4),0,22/5⁢(z+10⁢u2))⁢du.
36.9.7 |Ψ3⁡(x,y,z)|2 =27/451/4⁢∫0∞ℜ⁡(e2⁢i⁢u⁢(u4+z⁢u2+x)⁢Ψ2⁡(27/451/4⁢y⁢u3/4,2⁢u5⁢(3⁢z+10⁢u2)))⁢duu1/4.
36.9.8 |Ψ(H)⁡(x,y,z)|2=8⁢π2⁢(29)1/3⁢∫−∞∞∫−∞∞Ai⁡((43)1/3⁢(x+z⁢v+3⁢u2))×Ai⁡((43)1/3⁢(y+z⁢u+3⁢v2))⁢du⁢dv.
36.9.9 |Ψ(E)⁡(x,y,z)|2=8⁢π232/3⁢∫0∞∫02⁢πℜ⁡⁢(Ai⁡(131/3⁢(x+i⁢y+2⁢z⁢u⁢exp⁡(i⁢θ)+3⁢u2⁢exp⁡(−2⁢i⁢θ)))×Bi⁡(131/3⁢(x−i⁢y+2⁢z⁢u⁢exp⁡(−i⁢θ)+3⁢u2⁢exp⁡(2⁢i⁢θ))))×u⁢du⁢dθ.

For these results and also integrals over doubly-infinite intervals see Berry and Wright (1980). This reference also provides a physical interpretation in terms of Lagrangian manifolds and Wigner functions in phase space.