Diffraction Theory Illustrations

Jonathan Birge

MIT Ultrafast Optics and Quantum Electronics Group

Overview

In this Mathematica notebook, I illustrate the various approximations used in diffraction theory by focusing on the phase of the impulse responses (Green's functions) implicit in each. I intuitively show that Fraunhofer diffraction can be computed using the Fourier transform simply by arguing their equivalence from an impulse response standpoint. I also demonstrate the Fraunhofer diffraction approximation is actually completely conceptually separate from Fresnel diffraction and can be applied to any kernel, and furthermore, that it makes little sense to use the fresnel kernel as is typically shown in books. This will probably only be of much interest to people already briefly familiar with diffraction theory, though the pictures should serve as a nice illustration of what's going on with the approximations for somebody just learning diffraction theory.

This document is still pretty rough, so please feel free to e-mail me (birge at mit...) with any suggestions or questions, or if you'd like a copy of the actual Mathematica notebook.

Common Functions

This function will plot the phase fronts of a wave on a normalized set of axes. Assuming a wavenumber of one, we plot a few wavelengths in each direction just to make things look reasonable.

In[165]:=

In[191]:=

In[167]:=

Rect[x_]:=If[Abs[x]<1,1,0]

In[168]:=

PropagateSlit[kernel_,L_,x_,z_]:=NIntegrate[kernel[x-x0,z],{x0,-L,L}]

Spherical (Exact) Kernel

In scalar diffraction theory, the starting point is usually Huygen's principle, which states that the field emanating from an infinitely small point (i.e. the impulse response in 3D) is a spherical wave. This is needlessly vague and unrigorous. Even without dealing with equations (if anybody requests it, I'll go to the trouble of doing a proper derivation, but right now I doubt anybody will ever read this) one can do better. Starting from the full vector Maxwell equations, people commonly derive two fundamental wave solutions. The first is the usual plane wave that we're all familiar with. But when talking about computational diffraction these are not useful solutions, because it's difficult to match finite boundary conditions using waves with infinite extent. The other commonly derived solution to the wave equation is a spherical wave eminating from a point dipole. The transision to scalar diffraction is made by saying "well, if the aperture from which we're diffracting is large, the effects of the boundary conditions at the edge of the aperture will be small and won't differ with the polarization of the dipole." This, then, is the basis behind Huygen's principle. By considering all the points in the aperture as sources of spherical waves, you're doing the same thing electrical engineers do when they solve for the impulse response of a system and convolve it with a driving signal. The spherical solution to the wave equation is the impulse response (green's function) and the illuminated aperture is the driving function.

The phase of the impulse response is simply proportional to the distance from the slit (which we'll always assume to be at the origin). In the following plots, we'll just look at the phase, and we'll ignore the fact that the intensity also drops off in proportion to the distance in 2D. (This makes the plots easier to see, and all the interesting features of diffraction are described by the phase.)

In[169]:=

In[192]:=

Out[192]=

This is actually fine for computational diffraction, especially in two-dimensions (as shown here). The diffraction pattern of an arbitrary aperture can be approximated very quickly and yet accurately by computing the numerical approximation of the spatial convolution of the above kernel with the aperture. However, the radical makes anything but trivial situations impossible to compute analytically, as the integral that results from convolving the spherical wave with the aperture is usually unsolvable.

Given that we can easily compute diffraction patters with spherical waves, it's fair to ask why people go past this and on to Fresnel and Fraunhofer diffraction. The answer is partly historical and partly conceptual. But I will say this, however: Fresnel diffraction is completely practically useless. Fraunhofer diffraction is certainly useful as a conceptual tool, however, since the notion of a Fourier Transform is so powerful.

Fresnel Kernel

To make things simpler, Fresnel diffraction theory treats the spherical curvature to second-order along x, eliminating the radical:

In[171]:=

In[187]:=

Out[187]=

As you'd expect from a Taylor expansion, the approximation gets pretty bad away from the z-axis. It's valid as long as we're within a cone where the ratio of z to x is at least roughly the wavelength. As long as this requirement is satisfied, the result is valid regardless of the distance from the source. For this reason, Fresnel diffraction is also called "near-field" diffraction. (Of course, it's also valid arbitrarily far away, too.) The only problem is that it's still difficult to obtain analytic results for anything but completely contrived cases. Even a knife-edge can't be computed analytically. (Hence the so-called Fresnel function, which--as with all transcendental functions--is just mathematicians' way of saying we can't do the integral but would love to sound smart.)

What's the point?

It's simply historical and pedagogical. There are really no practical problems that can be solved analytically using Fresnel diffraction. And computationally, it's pretty much as difficult as using the more accurate spherical kernel. Thus, if you're going to use a computer to compute the near-field diffraction pattern you might as well use a spherical kernel.

Fraunhofer (Fourier) Diffraction

Fraunhofer Kernel Shifting

So, why is computing the diffraction pattern of arbitrary apertures with Fresnel diffraction difficult? The answer is that the resulting convolution integral is usually unsolvable in closed form, despite the simple form of the kernel. Apparently, it's just not simple enough of an impulse response to be of much use. (Just try yourself to compute the diffraction pattern from something as simple as a square function aperture.) Fortunately, there is another approximation that can be made if we assume that we are far enough from the source such that the source seems small, such that we never have to consider the kernel very far off axis during convolution.

Far away from the origin, small lateral shifts of the impulse response can be approximated by simply multiplying the kernel by an appropriate pure linear phase. That this is valid can be shown mathematically, and it can be intuitively argued from the point of view that the wavefronts a small distance from the z-axis are "tilted" an amount that is linearly proportional to the distance. This is simply the notion of a series expansion applied to the wavefront. So, the Fraunhofer approximation not only requires that we are in a region of large radius of curvature of the wavefronts, but also one where the aperture appears "small" so that we needn't consider the kernel very far off the x-axis. This latter requirement is why Fraunhofer diffraction is also called "far-field" diffraction since we must be far enough away for the source to be negligable in extent.

The amount of linear phase we need to add is proportional to the shift, Δx, as well as the slope to the location in the diffraction plane. For a unit displacement in our current normalized units, we have:

In[173]:=

If we multiply this phase by an unshifted Fresnel kernel, we should get something that looks just like the Fresnel kernel (at least far away from the source) but shifted down by one unit:

In[188]:=

Out[188]=

Compare this to the Fresnel kernel shifted by the same amount:

In[193]:=

Out[193]=

As you can see,the effect of simply multiplying by the linear phase term works really well except as you get too close to the source.

Fraunhofer Diffraction with Spherical Kernel

Something that never seems to be mentioned in books is that Fraunhofer diffraction is conceptually separate from Fresnel diffraction. At its core, Fraunhofer diffraction is simply a way of handling kernel shifts. It doesn't matter what we use for the static kernel in front of the linear phase term (so long as it works well within the Fraunhofer region). The paraxial approximations in Fresnel diffraction certainly lead nicely to Fraunhofer diffraction, and the latter is a subset of the former, but they are technically separate issues. Most importantly, the static kernel used will never have any interesting impact on the diffraction since it simply scales the intensity of the answer. Nonetheless, for the record, Fraunhofer diffraction can be done with any kernel, including the exact spherical kernel (though there's little advantage to doing so):

In[194]:=

Out[194]=

Fraunhofer Diffraction as Fourier Transform

With the Fraunhofer approximation, diffraction is treated as a linear system with an impulse response characterized by some static kernel multiplied by a complex exponential with a linear phase proportional to the shift. Since the static kernel (typically the Fresnel kernel) doesn't change with shifts, it can be moved outside of the convolution integral. So, at its heart, Fraunhofer diffraction is a linear system with a complex impulse response that is simply a complex exponential whose phase is proportional to the shift (delay) of the kernel times the distance from the origin: δ(x-Δx) → exp(i Δx α x/z), where α is some constant. A linear system is completely described by its impulse response (Green's function) so this is actually all we need to know about Fraunhofer diffraction. While not normally though of in such terms, the fact that an impulse function in space transforms to a complex exponential (in spatial frequency) completely describes the Fourier transform as a linear operation. Thus, Fraunhofer diffraction must simply be Fourier transformation multiplied by a static function. There are obviously details I've left out like the transformation of units (you can perhaps guess from the preceding that 'frequency' in the Fourier domain will have to be proportional to x/zλ) but the fundamental operation is the same.

Finally, then, we have a useful diffraction theory since the Fourier transform is so well known analytically, and so easily computed numerically. For example, despite the seemingly intractable complexity of computing the infinite interaction of waves eminating from a finite slit aperture, anybody with a transform table (or a copy of Mathematica) can deduce that the far-field diffraction pattern of such an aperture will be very nearly sin(x)/x.

Comparison of various approximations

What's interesting is that "Fraunhofer" diffraction with the spherical kernel is significantly better than diffraction with the fresnel kernel, especially far off-axis (where the quadratic approximation in the fresnel kernel breaks down). And yet it costs the same to compute. So, why do we use standard Fraunhofer diffraction with a fresnel kernel for cases where there is no analytic solution? (Note: since the kernel only appears in front of the integral in Fraunhofer diffraction, you might ask why it even matters, and its phase will drop out. In the case of a single aperture, it won't. But when considering multiple apertures, each of which can be computed with fraunhofer diffraction individually, but which violates the assumption as an ensemble, the kernels will interfere and it will matter.)

To see how using the spherical kernel might improve diffraction computations in the far field (essentially for free), consider the following plot.

In[202]:=

Out[202]=

This plot is a bit busy, but the main gist is this: the fraunhofer approximation works fine, even significantly off axis, in the sense that the shift is will approximated by the linear phase. However, relative to the exact solution (black) the fraunhofer with the spherical kernel works much better than the fresnel approximation for large angles. Surprisingly, there is even an advantage to the spherical kernel for small angles.

Page last edited:
February 06, 2008

Copyright 2003-2015 by
Jonathan R. Birge. All rights reserved.

Page generated:
18:23:30, October 17, 2017