Those quirky fermions

All of the matter in the universe is made of fermions. They are for this reason one of the most abundant things in the universe. Fermions have been the topic of investigation for a long time. We have learned much about them. However, what we do know about them is encapsulated in the formalisms with which we deal with them in our theories. Does that mean we understand them?

Let’s think about the way we treat fermions in our theories. Basically, we represent them in terms of creation and annihilation operators, which are used to formulate the interactions in which they take part. These operators are distinguished from those for bosons by the anti-commutation relations that they obey.

To the uninitiated, all this must sound like a bunch of gobbledygook. What are the physical manifestations of all these operators? There are none! These operators are just mathematical entities in the formalism for our theories. Although these theories are quite successful, it does not reveal the physical machinery at work on the inside. Or does it?

Although a creation operator does not by itself represent any physical process, it distinguishes different scenarios with different arrangements of fermions. Starting with a given scenario, I can apply a fermion creation operator to introduce a new scenario which contains one additional fermion. Then I can apply the operator again, provided that I am not trying to add another fermion with the same degrees of freedom, it will produce another new scenario.

Here is the strange thing. If I change the order in which I added the two additional fermions, I get a scenario that is different from the one with the previous order. I can contrast this to the situation with bosons. Provided that I don’t try to add bosons with the same degrees of freedom, the order in which I add them doesn’t matter. What it tells us is that bosons with different degrees of freedom don’t effect each other. (We need to be careful about the concepts of time-like or space-like separations, but for the sake of this argument, we’ll assume all bosons or fermions are space-like separated.)

The fact that the order in which we place fermions in our scenario (even when they are space-like separated) makes a difference tells us something physical about fermions. They must be global entities. The entire universe seems to “know” about the existence of each and every fermion in it.

How can that be possible? I can think of one way: topological defects. This is not a new idea. It pops up quite often in various fields of physics.

Topological defect

Why would a topological defect explain the apparent global nature of fermions? It is because all kinds of topological defects can be identified with the aid of an integral that computes the winding number of the topological defect. This type of integral is evaluated over a (hyper)surface that encloses the topological defect. In other words, the field values far away from the defect are included in the integral and not the field value at the defect. Therefore, knowledge about the defect in encoded in the entire field. It therefore suggest that fermions can behave as global entities if they topological defect. This is just a hypothesis. It needs more careful investigation.


Demystifying quantum mechanics V

Perhaps one of the most iconic “mysteries” of quantum mechanics is the particle-wave duality. Basically, it comes down to the fact that the interference effects one can observe implies that quantum entities behave like waves, but at the same time, these entities are observed as discrete lumps, which are interpreted as particles. Previously, I explained that one can relax the idea of localized lumps a bit to allow only the interactions, which are required for observations, to be localized. So instead of particles, we can think of these entities as partites that share all the properties of particles, accept that they are not localized lumps. So, they can behave like waves and thus give rise to all the wave phenomena that are observed. In this way, the mystery of the particle-wave duality is removed.

Now, it is important to understand that, just like particles, partites are discrete entities. The discreteness of these entities is an important aspect that plays a significant role in the phenomena that we observe in quantum physics. Richard Feynman even considered the idea that “all things are made of atoms” to be the single most important bit of scientific knowledge that we have.

Model of the atom

How then does it happen that some physicist would claim that quantum mechanics is not about discreteness? In her blog post, Hossenfelder goes on to make a number of statements that contradict much of our understanding of fundamental physics. For instance, she would claim that “quantizing a theory does not mean you make it discrete.”

Let’s just clarify. What does it mean to quantize a theory? It depends, whether we are talking about quantum mechanics or quantum field theory. In quantum mechanics, the processing of quantizing a theory implies that we replace observable quantities with operators for these quantities. These operators don’t always commute with each other, which then leads to the Heisenberg uncertainty relation. So the discreteness is not immediately apparent. On the other hand, in quantum field theory, the quantization process implies that fields are replaced by field operators. These field operators are expressed in terms of so-called ladder operators: creation and annihilation operators. What a ladder operator does is to change the excitation of a field in discrete lumps. Therefore, discreteness is clearly apparent in quantum field theory.

What Hossenfelder says, is that the Heisenberg uncertainty relationships is the key foundation for quantum mechanics. In one of her comments, she states: “The uncertainty principle is a quantum phenomenon. It is not a property of classical waves. If there’s no hbar in it, it’s not the uncertainty principle. People get confused by the fact that waves obey a property that looks similar to the uncertainty principle, but in this case it’s for the position and wave-number, not momentum. That’s not a quantum phenomenon. That’s just a mathematical identity.”

It seems that she forgot about Louise de Broglie’s equation, which relates the wave-number to the momentum. In a previous post, I have explained that the Heisenberg uncertain relationship is an inevitable consequence of the Planck and de Broglie equations, which relate the conjugate variables of the phase space with Fourier variables. It has nothing to do with classical physics. It is founded in the underlying mathematics associated with Fourier analysis. Let’s not allow us to be mislead by people that are more interested in sensationalism than knowledge and understanding.

The discreteness of partites allows the creation of superpositions of arbitrary combinations of such partites. The consequences for such scenarios include quantum interference that is observed in for instance the Hong-Ou-Mandel effect. It can also lead to quantum entanglement, which is an important property used in quantum information systems. The discreteness in quantum physics therefore allows it to go beyond what one can find in classical physics.

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