Airy function

In the physical sciences, the Airy function Ai(x) is a special function named after the British astronomer George Biddell Airy (1801–92). The function Ai(x) and the related function Bi(x), which is also called the Airy function, but sometimes referred to as the "Bairy" function, are solutions to the differential equation

\frac{d^2y}{dx^2} - xy = 0 , \,\!

known as the Airy equation or the Stokes equation. This is the simplest second-order linear differential equation with a turning point (a point where the character of the solutions changes from oscillatory to exponential).

The Airy function is the solution to Schrödinger's equation for a particle confined within a triangular potential well and for a particle in a one-dimensional constant force field. For the same reason, it also serves to provide uniform semiclasssical approximations near a turning point in the WKB method, when the potential may be locally approximated by a linear function of position. The triangular potential well solution is directly relevant for the understanding of many semiconductor devices.

The Airy function also underlies the form of the intensity near an optical directional caustic, such as that of the rainbow. Historically, this was the mathematical problem that led Airy to develop this special function.

Contents

Definitions

Plot of Ai(x) in red and Bi(x) in blue.

For real values of x, the Airy function is defined by the improper integral

\mathrm{Ai}(x) = \frac{1}{\pi} \int_0^\infty \cos\left(\tfrac13t^3 + xt\right)\, dt,

which converges because the positive and negative parts of the rapid oscillations tend to cancel one another out (as can be checked by integration by parts).

By differentiating under the integration sign, we find that y = Ai(x) satisfies the differential equation

y'' - xy = 0 . \,\!

This equation has two linearly independent solutions. The standard choice for the other solution is the Airy function of the second kind, denoted Bi(x). It is defined as the solution with the same amplitude of oscillation as Ai(x) as x goes to −∞ which differs in phase by π/2:

\mathrm{Bi}(x) = \frac{1}{\pi} \int_0^\infty \left[\exp\left(-\tfrac13t^3 + xt\right) + \sin\left(\tfrac13t^3 + xt\right)\,\right]dt.

Properties

The values of Ai(x) and Bi(x) and their derivatives at x = 0 are given by

\begin{align}
 \mathrm{Ai}(0) &{}= \frac{1}{3^{2/3}\Gamma(\tfrac23)}, & \quad \mathrm{Ai}'(0) &{}= -\frac{1}{3^{1/3}\Gamma(\tfrac13)}, \\
 \mathrm{Bi}(0) &{}= \frac{1}{3^{1/6}\Gamma(\tfrac23)}, & \quad \mathrm{Bi}'(0) &{}= \frac{3^{1/6}}{\Gamma(\tfrac13)}.
\end{align}

Here, Γ denotes the Gamma function. It follows that the Wronskian of Ai(x) and Bi(x) is 1/π.

When x is positive, Ai(x) is positive, convex, and decreasing exponentially to zero, while Bi(x) is positive, convex, and increasing exponentially. When x is negative, Ai(x) and Bi(x) oscillate around zero with ever-increasing frequency and ever-decreasing amplitude. This is supported by the asymptotic formulae below for the Airy functions.

The Airy functions are orthogonal[1] in the sense that

 \int_{-\infty}^\infty \mathrm{Ai}(t+x) \mathrm{Ai}(t+y) dt = \delta(x-y).

Asymptotic formulae

The asymptotic behaviour of the Airy functions as x goes to +∞ is given by the following asymptotic formulae:[2]

\begin{align}
 \mathrm{Ai}(x) &{}\sim \frac{e^{-\frac{2}{3}x^{3/2}}}{2\sqrt\pi\,x^{1/4}} \\[6pt]
 \mathrm{Bi}(x) &{}\sim \frac{e^{\frac{2}{3}x^{3/2}}}{\sqrt\pi\,x^{1/4}}.
\end{align}

For the limit in the negative direction we have[3]

\begin{align}
 \mathrm{Ai}(-x) &{}\sim \frac{\sin \left(\frac23x^{3/2}+\frac14\pi \right)}{\sqrt\pi\,x^{1/4}} \\[6pt]
 \mathrm{Bi}(-x) &{}\sim \frac{\cos \left(\frac23x^{3/2}+\frac14\pi \right)}{\sqrt\pi\,x^{1/4}}. 
\end{align}

Asymptotic expansions for these limits are also available. These are listed in (Abramowitz and Stegun, 1954) and (Olver, 1974).

Complex arguments

We can extend the definition of the Airy function to the complex plane by

\mathrm{Ai}(z) = \frac{1}{2\pi i} \int_{C} \exp\left(\tfrac{1}{3}t^3 - zt\right)\, dt,

where the integral is over a path C starting at the point at infinity with argument -(1/3)π and ending at the point at infinity with argument (1/3)π. Alternatively, we can use the differential equation y'' − xy = 0 to extend Ai(x) and Bi(x) to entire functions on the complex plane.

The asymptotic formula for Ai(x) is still valid in the complex plane if the principal value of x2/3 is taken and x is bounded away from the negative real axis. The formula for Bi(x) is valid provided x is in the sector {xC : |arg x| < (1/3)π−δ} for some positive δ. Finally, the formulae for Ai(−x) and Bi(−x) are valid if x is in the sector {xC : |arg x| < (2/3)π−δ}.

It follows from the asymptotic behaviour of the Airy functions that both Ai(x) and Bi(x) have an infinity of zeros on the negative real axis. The function Ai(x) has no other zeros in the complex plane, while the function Bi(x) also has infinitely many zeros in the sector {zC : (1/3)π < |arg z| < (1/2)π}.

Plots

\Re \left[ \mathrm{Ai} ( x + iy) \right] \Im \left[ \mathrm{Ai} ( x + iy) \right] | \mathrm{Ai} ( x + iy) | \, \mathrm{arg} \left[ \mathrm{Ai} ( x + iy) \right] \,
AiryAi Real Surface.png AiryAi Imag Surface.png AiryAi Abs Surface.png AiryAi Arg Surface.png
AiryAi Real Contour.svg AiryAi Imag Contour.svg AiryAi Abs Contour.svg AiryAi Arg Contour.svg
\Re \left[ \mathrm{Bi} ( x + iy) \right] \Im \left[ \mathrm{Bi} ( x + iy) \right] | \mathrm{Bi} ( x + iy) | \, \mathrm{arg} \left[ \mathrm{Bi} ( x + iy) \right] \,
AiryBi Real Surface.png AiryBi Imag Surface.png AiryBi Abs Surface.png AiryBi Arg Surface.png
AiryBi Real Contour.svg AiryBi Imag Contour.svg AiryBi Abs Contour.svg AiryBi Arg Contour.svg

Relation to other special functions

For positive arguments, the Airy functions are related to the modified Bessel functions:

\begin{align}
 \mathrm{Ai}(x) &{}= \frac1\pi \sqrt{\frac13 x} \, K_{1/3}\left(\tfrac23 x^{3/2}\right), \\
 \mathrm{Bi}(x) &{}= \sqrt{\frac13 x} \left(I_{1/3}\left(\tfrac23 x^{3/2}\right) + I_{-1/3}\left(\tfrac23 x^{3/2}\right)\right).
\end{align}

Here, I±1/3 and K1/3 are solutions of x2y'' + xy' − (x2 + 1 / 9)y = 0.

The first derivative of Airy function is

  \mathrm{Ai'}(x) = - \frac{x} {\pi \sqrt{3}} \, K_{2/3}\left(\tfrac23 x^{3/2}\right) .

Functions K1 / 3 and K2 / 3 can be represented in terms of rapidly converged integrals[4] (see also modified Bessel functions )

For negative arguments, the Airy function are related to the Bessel functions:

\begin{align}
 \mathrm{Ai}(-x) &{}= \frac13 \sqrt{x} \left(J_{1/3}\left(\tfrac23 x^{3/2}\right) + J_{-1/3}\left(\tfrac23 x^{3/2}\right)\right), \\
 \mathrm{Bi}(-x) &{}= \sqrt{\frac13 x} \left(J_{-1/3}\left(\tfrac23 x^{3/2}\right) - J_{1/3}\left(\tfrac23 x^{3/2}\right)\right). \end{align}

Here, J±1/3 are solutions of x2y'' + xy' + (x2 − 1 / 9)y = 0.

The Scorer's functions solve the equation y'' − xy = 1 / π. They can also be expressed in terms of the Airy functions:

\begin{align}
 \mathrm{Gi}(x) &{}= \mathrm{Bi}(x) \int_x^\infty \mathrm{Ai}(t) \, dt + \mathrm{Ai}(x) \int_0^x \mathrm{Bi}(t) \, dt, \\
 \mathrm{Hi}(x) &{}= \mathrm{Bi}(x) \int_{-\infty}^x \mathrm{Ai}(t) \, dt - \mathrm{Ai}(x) \int_{-\infty}^x \mathrm{Bi}(t) \, dt. \end{align}

Fourier transform

Using the definition of the Airy function Ai(x), it is straightforward to show its Fourier transform is given by


\mathcal{F}(\mathrm{Ai})(k) := \int_{-\infty}^{\infty} \mathrm{Ai}(x)\ \mathrm{e}^{- 2\pi \mathrm{i} k x}\,dx =
\mathrm{e}^{\frac{\mathrm{i}}{3}(2\pi k)^3}\,.

History

The Airy function is named after the British astronomer and physicist George Biddell Airy (1801–1892), who encountered it in his early study of optics in physics (Airy 1838). The notation Ai(x) was introduced by Harold Jeffreys. Airy had become the British Astronomer Royal in 1835, and he held that post until his retirement in 1881.

Notes

  1. ^ David E. Aspnes, Physical Review, 147, 554 (1966)
  2. ^ Abramowitz & Stegun (1970), Eqns 10.4.59 and 10.4.63
  3. ^ Abramowitz & Stegun (1970), Eqns 10.4.60 and 10.4.64
  4. ^ M.Kh.Khokonov. Cascade Processes of Energy Loss by Emission of Hard Photons // JETP, V.99, No.4, pp. 690-707 \ (2004).

References

External links


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