The idea that a particle could pass through a wall by luckily avoiding collisions is a classical way of thinking. In that view, a particle is a tiny solid ball and a wall is just a collection of other tiny balls with space between them.
Quantum tunneling is based on a completely different concept. In quantum mechanics, the "wall" is not a physical object but a high energy barrier. Classically, a particle cannot be in a region if it doesn't have enough energy to overcome that barrier (this is why people often use the idea of a high wall and a ball that cannot make it over the wall). However, quantum mechanics treats particles as having wave-like properties. This wave is related to the probability of finding the particle at any given location. While the probability of finding the particle inside the high-energy barrier is very low, it is not zero. The wave's amplitude shrinks inside the barrier, but a small portion of it extends to the other side. This means there is a small but finite probability that if you measure the particle's position, you will find it on the other side. When that happens, we say the particle has "tunneled" through.
The surprising success of the experiments that led to the Nobel Prize today is that it wasn’t just a single particle (like an electron) that they measured tunneling through a barrier, it was a macroscopic group of particles. These particles were able to tunnel through the barrier because they were kept in a coherent state that allowed them to have a wave function that coherently extended through the barrier. This meant that they had a reasonable finite amplitude on the other side of the barrier so that a measurement could show that they tunneled through the barrier.
Thanks, I'm still thinking about your answer but really appreciate your explanation. Would this mean that there is some (possibly currently unknown) maximum size for a group of particles that could be forced to maintain the correct state to pass through the wall?
This is another great question. It's still a matter of debate how the wave-like behavior of quantum mechanics turns into the particle-like behavior of large objects that we observe. Some people believe there should be a maximum size, some people believe that there isn't. In fact Nature did a survey a few months ago and found that physicists disagree wildly on this topic. https://www.nature.com/articles/d41586-025-02342-y
Have you heard of Schrodinger's cat, which is hypothetically dead and alive at the same time? Schrodinger described this thought experiment to argue that quantum mechanics led to absurdities if you took it too far. Ironically, many physicists now believe that such an experiment is possible in principle, though it would be extremely difficult.
There is no obvious limit to how big you could scale up this experiment right here. In practice, these circuits are already big enough that you can quite literally see them with the naked eye (~mm in length). Nothing really stops you from making one meters in diameter, aside from the obvious impracticality of cooling such a massive structure to the required temperature. Nobody expects this to break any known physics by doing so. In fact, some of these experiments have also been used to estimate lower bounds for nonlinear versions of quantum mechanics (where collapse is a real thing, and the larger an object is, the faster it collapses).
But you should not really think of a physical wall in this case. The experiments that have proven the macroscopic tunneling behave according to the same exact math, but nothing is really tunneling through macroscopic walls. The cooper pair electrons are, but that’s a different Nobel prize (Josephson, 1973).
The real limit is not based on the size or number of particles, but on the coherence of the group of particles. Using the word coherence is probably not helpful without context, so let me give a quick explanation of what that means.
As I mentioned in my answer above, particles can exhibit wave-like properties. A group of particles will each have their own wave packet. In our everyday lives, two particles, even those right next to each other, are jiggling around randomly due to temperature and experiencing slightly different environments. You can think of each of these separate random jiggles as a measurement that collapses the wave function of that particle. Then, after the particle's wave function collapses, it begins to evolve again until the next measurement. As a side note, saying a measurement collapses the wave function is quantum mechanics talk for the observed reality that when we measure where a particle is, we do not find a wave, we find a particle. So, the shorthand for this view of quantum mechanics is that a measurement collapses the wave function.
Ok, so now we have a bunch of particles, like a chair. Why won't a chair tunnel through a wall? Well, all the particles that make up the chair are not just physically separated, but they are jiggling due to their temperature and their slightly different environments. So, all of these particles that make up the chair keep having their wave function collapsed randomly. The chance of one particle tunneling through the wall is small. The chance of all 10^27 particles in the chair independently tunneling through the barrier at once is not going to happen before the universe ends.
Back to coherence. All of these particles of the chair are independently jiggling around, and each one has its own wave function collapsed very quickly. For this reason, you can treat each particle as an independent particle. We would say the wave functions of these particles are not coherent with each other.
Now, imagine that we have two particles right next to each other. At room temperature, they are constantly jiggling and having their wave functions collapsed. If we cool them down to reduce the jiggling, and they are close enough to each other, their respective wave functions can start to overlap. When the jiggling of the particles is small enough and their wave functions overlap sufficiently, they begin to behave as a single quantum entity. This is a coherent state. In a suitably constructed experiment, these coherent particles can then exhibit quantum behaviors such as tunneling together.
Back to your question: is there some maximum size for a group of particles that could be forced to maintain the correct state to pass through the wall? Since the group of particles must be in a coherent quantum state to tunnel, the real question is how big of a group can be put into such a state. You have to cool them to slow the jiggling, isolate them from anything in the environment that might collapse their wave functions, and get them close enough together for their wave functions to overlap. There is likely a theoretical limit that could be calculated, but as a practical matter, extraordinary engineering efforts are required to get even a very small group of particles into a coherent quantum state. The direct answer to your question is that while there may be a theoretical maximum possible size of a coherent state for our universe, the real limit is set by the immense practical challenges of creating and maintaining a coherent state. This is what makes the work of this year’s Nobel Prize winners so impressive.
Does a denser wall produce a higher-energy barrier?
And, if so, is there then actually a practical difference between the classical and quantum interpretations? (i.e. could it simply be said that, the denser wall just has more chances to collide with the particle and stop it from passing through, thus explaining why the probability of finding it on the other side is lower?)
The idea that a particle could pass through a wall by luckily avoiding collisions is a classical way of thinking. In that view, a particle is a tiny solid ball and a wall is just a collection of other tiny balls with space between them.
Quantum tunneling is based on a completely different concept. In quantum mechanics, the "wall" is not a physical object but a high energy barrier. Classically, a particle cannot be in a region if it doesn't have enough energy to overcome that barrier (this is why people often use the idea of a high wall and a ball that cannot make it over the wall). However, quantum mechanics treats particles as having wave-like properties. This wave is related to the probability of finding the particle at any given location. While the probability of finding the particle inside the high-energy barrier is very low, it is not zero. The wave's amplitude shrinks inside the barrier, but a small portion of it extends to the other side. This means there is a small but finite probability that if you measure the particle's position, you will find it on the other side. When that happens, we say the particle has "tunneled" through.
The surprising success of the experiments that led to the Nobel Prize today is that it wasn’t just a single particle (like an electron) that they measured tunneling through a barrier, it was a macroscopic group of particles. These particles were able to tunnel through the barrier because they were kept in a coherent state that allowed them to have a wave function that coherently extended through the barrier. This meant that they had a reasonable finite amplitude on the other side of the barrier so that a measurement could show that they tunneled through the barrier.