What’s in a Particle?

photon identity crisis
This photon doesn’t know whether it’s a particle or a wave. (Unknown source.)

If you’ve read or heard anything about quantum mechanics, you’ve heard the phrase “particle-wave duality.” The common wisdom is that this means that particles sometimes behave like waves and sometimes behave like particles. And although this is right, it’s a bit misleading. The truth is:

Everything is always a wave. It’s just that waves can be made to behave like particles.

To see what I mean, let’s actually show how one can make a set of waves behave like a particle. Specifically, let’s show how a set of light waves can be made to behave like a photon, a light particle.

Light Goes Round

Just to be concrete, let’s talk about light that bounces between a special configuration of mirrors. It looks something like this:

a ring cavity
The configuration of mirrors we’re considering. The light (yellow) starts at mirror A (light blue), bounces off of mirrors B and C, and ends up back where it started. The process repeats forever.

The idea is to configure three mirrors (light blue) so that the light (yellow) bounces around in a loop so that it ends up in the same place that it started from. In optics, this is called a ring cavity. It’s often used to make a type of laser called a ring laser.

We can represent the path of the light (which lives in two-dimensions) as a position along a single line. All we have to do is demand that the lefthand side of the line be the same point as the righthand side of the line so that it wraps around to where it started, as shown below. This is called a periodic representation.

ring-cavity-flattened
The ring cavity reduced to a single line so that the path of the light starts at the left and ends on the right… the left and right points represent the same point.

So, given our periodic plot of the path of the light in the cavity, what does a light wave look like? Since the wave has to wrap around to where it started, the wave on the left side of the line must look the same as it does on the right… In other words, it has to become itself after it travels around the cavity, as shown below:

sine it!
A sine wave in the ring cavity. The left side of the wave looks the same as the right because it must be periodic.

One important consequence of this periodicity is that the waves in the cavity can’t be whatever they want. Only certain waves fit. In the figure above, if the wave stopped a little earlier on the right (say at the peak, the highest point), as shown below, then the right and left sides of the wave wouldn’t be the same. This would obviously be a problem.

sinfivex_trunc
This wave doesn’t fit in our ring cavity because the left and right sides are not the same.

 

Now, given a bunch of light waves that fit in our cavity, we want to combine them in such a way that we get a particle travelling around the ring in the cavity. An important idea that we’ll need is the principle of superposition. 

The Superposition Principle

I’ve previously discussed wave interference and the superposition principle, so if you remember my previous discussions, feel free to skip to the next section.

Imagine waves as wiggles on a very stretchy string. If I try and push up on the string (make a wiggle that goes up) and you try and push down on the string (make a wiggle that goes down) at the same time, neither of us ends up moving the string as much as we intended. This is called destructive interference. Similarly, if I push up on the string at the same time that you push up on the string, we’ll probably stretch it quite a lot. This is called constructive interference. The process of overlaying one wave over another is called superposition.

Interference between two waves on a string
If we both try to make waves on a string, we may interfere with each other. If, as in the image on the left, we both try making the same wave, we may get a bigger wave than we intended. This is called constructive interference. If, on the other hand, we try to make waves exactly offset from each other, we may completely negate each others’ efforts. This is called destructive interference (source).

Light waves work the same way. If we make two waves overlap

What’s in a Particle

Okay, so let’s build our particle! As a first step, let’s put the largest wave that can possibly fit into our cavity, shown below. Note how the height of the wave on the left is always the same as the height of the wave on the right.

ring_cavity_n1
A single, low-frequency, wave travelling through a ring cavity.

Now, we add more, higher frequency, waves to the cavity. (By higher-frequency, I mean the waves have more wiggles in them.) If we take a wave that has exactly twice the number of wiggles as our first wave and add the two waves together, we get something like this:

ring_cavity_n2
Two waves superposed in the ring cavity. Already we start to see some particle-like structure.

Interesting! Now we get a big wiggle and a small wiggle. Perhaps that big wiggle will become a particle?

(Note that I added a wave of a specific height to the first wave. There’s a lot of math involved in knowing precisely what height to add. I’m going to completely ignore that detail for now.)

After we add five waves to the cavity and sum up the wiggle heights, we get:

ring 5
Five waves superposed in the ring cavity.

Now there’s one wiggle that’s clearly much bigger than the others. If we add enough waves to the cavity, we can make that wiggle all we can see:

ring_cavity_n20
20 waves superposed in a ring cavity.

Wow! That doesn’t even look like a wave! What is that? That, my friends, is a particle. The point where the peak is highest represents the average position of the particle and the width of the peak represents the quantum uncertainty in the position of the particle.

(Actually, the little wiggles around the peak are still there. They’re just too small to see in my plot. In principle, you can get rid of them entirely by adding up infinitely many waves.)

Enter Heisenberg

What if we wanted to make the peak narrower, thus making it possible to measure the particle’s position more precisely? Well, you might have noticed that our central peak got narrower as we added more waves to our ring cavity. This means that we would need to add more, increasingly wiggly, waves to the cavity to make the peak narrower.

How do we interpret that? We know that the number of wiggles in a wave determines both its energy and its momentum, meaning that the particle is not only made up of many waves, but has many different energies.

It has an average energy, of course, and an average momentum. But if we measure the particle, we might not measure that energy or that momentum. Instead, we’ll measure each energy some fraction of the time. The percentages look something like this:

energy-distribution
The percentage of the particle that has a given energy.

This is a visible manifestation of the Heisenberg uncertainty principle. If we want to know the particle’s position better, we need to add waves with different energies to it, meaning that it has more energies and we know the energy (and thus the momentum) less well.

Particles Can Act Like Waves

So I’ve just described how we can make a bunch of waves like a particle. But, of course, a bunch of particles can wiggle to make a wave. This is, after all, what’s going on when you wiggle a string, since that string is made up of particles. So you might ask… can you make a wave out of particles, add a bunch of such waves together, and get a new particle?

Amazingly, you can! If you add up a bunch of sound waves travelling through a material (which is made of particles which are made up of waves), you can get a particle called a phonon!

So now we’re ready to state the principle of particle-wave duality one last time:

Everything is a wave. But particles can be constructed out of waves… and waves can be constructed out of particles.

Disclaimer: It’s Often Useful to Think in Terms of Particles

I just told you everything is a wave. But that doesn’t mean physicists always think in terms of waves. Often it’s more useful to think in terms of particles. For example, the width of the peak I constructed above can be very narrow on human terms and it can be very difficult to notice or measure uncertainty in the particle’s position. This is why we didn’t discover quantum mechanics until the early twentieth century.

But even at the quantum level, it’s often valuable to think in terms of particles. Richard Feynman’s diagrams, and Werner Heisenberg’s formulation of quantum mechanics, for example, treat particles as particles in some sense. This isn’t inconsistent, however, because one can prove that Feynman and Heisenberg’s formulations imply the wave nature of, well, Nature.

Alright folks, that’s all I have for now.

Play With it Yourself

I generated all of my animations in Python. If you’d like to play with them yourself, you can find my code here:

https://github.com/Yurlungur/make-a-particle

Related Reading

I’ve written about quantum mechanics before. If you enjoyed this post, you might also enjoy the following posts:

  • In this article, I introduce particle-wave duality by describing the experiments that convinced physicists that particles have to be waves.
  • In this article, I describe how Niels Bohr used particle-wave duality to unravel the mysteries of the atom.
  • In this article, I explain how we should interpret particles-as-waves.
  • In this article, I use particle-wave duality to explain quantum tunneling.
  • Everything I just described is based on something called Fourier Analysis. I discuss Fourier analysis in a very similar context in this article.

6 thoughts on “What’s in a Particle?

  1. Can you kindly explain: does energy move from A -> B -> C -> A in a wavy fashion, i.e. not on a straight line, or does the wave represent changes in the intensity of an energy field?
    In other words what moves and how?

    1. Hi Andrea,

      I’m so sorry for the late reply! It seems my email notifications for comments are being sent to my spam folder!

      The energy moves in a straight line. The wave represents the strength of an electric field. You can also think of the square of the height of the wave as representing measuring a probability at some position.

  2. I am forever confused by the representation of a light wave in 2-dimensions. Does a light wave not fluctuate in all 3-dimensions? When light is emitted from a source such as a light bulb, it is emitted in all directions in all three spaces so what keeps each wave from cancelling out other waves right next to it?

    1. Hi Vince,

      I’m so sorry for the late reply! It seems my email notifications for comments are being sent to my spam folder!

      A wave usually travels in 3 dimensions but only “fluctuates” in two of them, which are perpendicular to the direction of travel. You’re absolutely right that representing a light wave in 2 dimensions isn’t quite right… but I chose to do it for the sake of clarity. (As you can tell, it gets confusing!)

      In answer to your question about light emitted from a light bulb, the waves do cancel each other out to some extent… some parts get cancelled out and some parts add up. The fluctuations form what’s called a “spherical” wave.

  3. Hi Vince,

    I’m so sorry for the late reply! It seems my email notifications for comments are being sent to my spam folder!

    A wave usually travels in 3 dimensions but only “fluctuates” in two of them, which are perpendicular to the direction of travel. You’re absolutely right that representing a light wave in 2 dimensions isn’t quite right… but I chose to do it for the sake of clarity. (As you can tell, it gets confusing!)

    In answer to your question about light emitted from a light bulb, the waves do cancel each other out to some extent… some parts get cancelled out and some parts add up. The fluctuations form what’s called a “spherical” wave.

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