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Some electronics textbooks seem to refer to holes as just a construct, while solid state physics textbooks seem to imply that holes are a very real thing. I understand that holes are vacancies (p-n junctions) that move towards the cathode while electrons move towards the anode, however, is a hole a real thing, or is it just a construct? I just want to think of it as a construct but I want to hear the general consensus. For example, recombination occurs in a semiconductor when an electron fills a hole.

What exactly is meant, then, when a photon is absorbed in semiconductor (e.g. a silicon p-i-n photodetector absorbs a lower-energy visible red photon about 400 nm within its band gap energy). When the semiconductor absorbs the photon, it cannot simply convert to an electron because charge, spin and lepton number would be violated. Is it converting into an electron and hole, and is a hole an actual, elemental particle? Does it make sense that an electron and hole move in opposite directions towards the anode and cathode, respectively, when radiative absorption occurs?

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    $\begingroup$ the word "fundamental particle" is reserved for the particles in the standard model of particle physics en.wikipedia.org/wiki/Standard_Model . The electron is one of them and its existence does not depend on a medium. $\endgroup$ – anna v Dec 2 '17 at 10:16
  • $\begingroup$ As Anna said. You cannot think of a hole without a medium or a construction. $\endgroup$ – Alchimista Dec 2 '17 at 10:29
  • $\begingroup$ Thanks, that's what I thought. Then how are charge, spin and lepton number conserved when a photon is captured in a photovoltaic/photodetector or emitted in a light emitting diode? Simply the release of an electron neutrino or antineutrino? Does that have any practical implications for photodetectors/LEDs? $\endgroup$ – DrNormal Dec 4 '17 at 0:08
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To adress the question of yours about conservation of charge / lepton number / spin: The definition of a "hole" as the absence of an electron requires there to be many electrons "arround". Whenever something is the absence of something else, this means that the presence of something is the default. You can as well identify a hole in a paper, because there is paper arround, but you wouldn't point into the sky and say "Oh look! A Paper hole". It's the same with electrons: In the scenario you described, you have to think about that there are many electrons in the crystal, occupying different states (quantum mechanical states) $|\Psi_{\vec{k}}\rangle$. The Photon will excite one of those electrons $|\Psi_{\vec{k_0}}\rangle$, bringing it to a different state $|\Phi\rangle$. You then have one excited electron, and one hole in the entirety of other states.

Your other question asked wether this notion of holes is all that there is about this topic. It is not:

Think about this: Imagine electrons as little balls with finite diameter, being at rest, for example arranged in a squared pattern. Take one of those Balls away. This is your hole. Now you apply an electric field, which will accelerate all balls to the left. What happens to your hole? Right, it accelerates to the left as well. This is not the behaviour you expect from the semiconductor holes, which are supposed to mimic positive charges in every possible way.

To explain the semiconductor wholes, we have to get back to the "entirety of states $\Psi_{\vec{k}, n}$, mentioned before. Also, we need something that is called band-structure. And we need Schrödingers equation. It's solutions in a semiconductor can be denoted by $|\Psi_{\vec{k},n}\rangle$, where n denotes the that called band. For each band n, there is a class of states $|\Psi_{\vec{k},n}\rangle$ that satisfies Schrödingers equation with Energies $E(\vec{k})$. enter image description here

This picture shows $E(\vec{k})$ pretty well. What is important is that the classical properties of the electron (like accelleration) behave as if they had a mass which is proportional to the second derivative of $E(\vec{k})$. This is called effective mass. The next thing is: The states are usually filled up from the lowest energy to the highest. Assume that one of the lower energy bands in the picture is completely filled up with electrons. Now one electron is excited by a photon to one of the higher energy "bands" (which would be the highes parabola in the picture). The single electron being in the higher-energy-band does sit somewhere near $\vec{k}=0$. The parabola does have a positive second derivative here (which means a positive effective mass). Now look at the hole: It is at maximum of the lower parabola, and does have negative effective mass. Thus applying an electric field will accellerate it to a direction you would expect a positive charge to accellerate to.

Long story short: In semiconductor physis, a hole isn't just the absence of an electron, but a certain state of a quantum mechanical many-body system, which doesn't behave like the absence of an electron at all.

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  • $\begingroup$ Thanks, reading your answer made me realize how stupid my question & how I completely forgotten some key concepts! The photon is being absorbed by the Si atom (much like the well-known spectral absorption lines of hydrogen), thus, the photon is being 'eaten' by the atom, if you will, & its energy is going into exciting the electron orbital by boosting a valence electron into the bottom of the conduction band. The photon has no charge or lepton number, and its spin is conserved in the new excited atomic orbital state. No electrons are created; the free electron simply leaves a hole behind. $\endgroup$ – DrNormal Dec 6 '17 at 2:05
  • $\begingroup$ and yeah, the hole is more than just the absence of an electron, because it disrupts the bloch wavefunction/periodic potential, so it is effectively a many-body state. A hole is, in fact, a many-body state of many electrons in a crystal lattice, so a hole needs both electrons and a lattice to exist (like you said you don't say, "Oh look, there's a paper hole in the sky.") It is absolutely not a fundamental particle whatsoever; it is a construct, or a superposition of electrons in a disturbed periodic potential. $\endgroup$ – DrNormal Dec 6 '17 at 2:17
  • $\begingroup$ @Quantumwhisp-One minor point. You write: **Think about this: Imagine electrons as little balls with finite diameter, being at rest, for example, arranged in a square pattern. Take one of those balls away. This is your hole. Now you apply an electric field, which will accelerate all balls to the left.What happens to your hole? Right, it accelerates to the left as well. ** But won't the hole accelerate in the opposite direction as the ball (the electron) does, i.e. to the right? $\endgroup$ – descheleschilder Dec 19 '17 at 1:56
  • $\begingroup$ @descheleschilder If you imagine the hole simply as the absence of a "ball", then no, it will acellerate to the left as all the balls arround do. Because of this, the naive picture of a hole simply being "the absence of an electron" doesn't give an explanation why holes would behave like positive charges. To explain the observed behaviour of holes (that would be acellerating to the right), you have to do all the many-particle / effective mass trickery I mentioned. $\endgroup$ – Quantumwhisp Dec 19 '17 at 11:46
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Holes can be understood as nothing but vacant orbitals, and a consider holes aren't elemental particles.

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