Another photoelectric effect related question

In summary, the photoelectric effect is not limited to visible light and can also occur with UV sources. When photons have energy greater than the work function, electrons from the top of the conduction band can be liberated with high kinetic energy. As the energy of the photons increases, more complicated processes such as core-level photoemission and Auger processes may occur. The recoil momentum is taken up by the lattice.
  • #1
N00bDaan
1
0
Hi,

After searching the forum I did not find an answer to my question, so here goes.

In the classical theory a photon can only eject a photo electron when the energy of the photon is greater than the binding energy of the electron. This is only possible with bound electrons as some of the recoil momentum has to be taken over by the nucleus.

The photoelectric effect was observed with visible light and a metal. I assume that the photo electrons emitted from a metal by visible light are actually electrons originating from the conductance band (CB) as the photon energy is quite low. This also means that the recoil momentum is actually taken over by the crystal lattice of the metal. Is this correct?

When the incident photons far greater energy and we still try to eject photoelectrons from a metal what will happen? I think that no electrons from the CB will be ejected and, depending on the energy, bound electrons will be ejected because the recoil momentum can now only be taken over by the nucleus. Or will there also be electrons emitted from the CB (now with far greater kinetic energy)? Is related to the atomic cross-section of the photoelectric effect?

Someone with some input?
 
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  • #2
N00bDaan said:
Hi,

After searching the forum I did not find an answer to my question, so here goes.

In the classical theory a photon can only eject a photo electron when the energy of the photon is greater than the binding energy of the electron. This is only possible with bound electrons as some of the recoil momentum has to be taken over by the nucleus.

The photoelectric effect was observed with visible light and a metal. I assume that the photo electrons emitted from a metal by visible light are actually electrons originating from the conductance band (CB) as the photon energy is quite low. This also means that the recoil momentum is actually taken over by the crystal lattice of the metal. Is this correct?

When the incident photons far greater energy and we still try to eject photoelectrons from a metal what will happen? I think that no electrons from the CB will be ejected and, depending on the energy, bound electrons will be ejected because the recoil momentum can now only be taken over by the nucleus. Or will there also be electrons emitted from the CB (now with far greater kinetic energy)? Is related to the atomic cross-section of the photoelectric effect?

Someone with some input?

First of all, the "photoelectric effect" doesn't just apply to visible light. One can also do this with UV sources, and in fact, that's what you will need if you want to see this effect on something like copper, which has a work function of around 4.7 eV.

When the photons have energy far greater than the work function, a number of things can happen. You can still get electrons from the top of the conduction band (near the Fermi level), and these electrons will be liberated with a lot of kinetic energy. For example, look at a typical photoemission spectrum. You'll see a plenty of electrons at the high energy tail end of the spectrum. You can also start getting photoelectrons that came deeper from the conduction band.

Beyond that, things start to get complicated. Depending on the skin depth of that particular photon frequency and the material, one can also start to get core-level photoemission. This is where the photoelectrons came not from the conduction band, but from the bound state of the atoms/molecules that made up the material. One can also start to get Auger processes where this is now no longer a "photoemission" process.

And yes, the recoil momentum is taken up by the lattice.

Zz.
 
  • #3


Hello,

Thank you for your question about the photoelectric effect. It is a very interesting topic in the field of quantum mechanics.

You are correct in your understanding that in the classical theory, a photon can only eject a photoelectron when the energy of the photon is greater than the binding energy of the electron. In the photoelectric effect, the incident photon transfers its energy to an electron in the metal, causing it to be ejected from the surface. This is only possible with bound electrons as the recoil momentum has to be taken over by the nucleus.

When visible light is used, the photon energy is relatively low, so the electrons being ejected are mostly from the conduction band. However, as you mentioned, when the incident photons have much greater energy, bound electrons may also be ejected. This is because the energy of the photon can now overcome the binding energy of the electron and cause it to be ejected.

In this case, the recoil momentum can only be taken over by the nucleus, as you mentioned. This can result in electrons being emitted from the conduction band with greater kinetic energy, as well as bound electrons being ejected. The atomic cross-section of the photoelectric effect plays a role in determining the likelihood of electrons being ejected from the conduction band or the bound electrons.

I hope this helps to clarify your understanding of the photoelectric effect. If you have any further questions, please don't hesitate to ask. Keep exploring and learning about this fascinating phenomenon!
 

Related to Another photoelectric effect related question

1. What is the photoelectric effect?

The photoelectric effect is a phenomenon in which electrons are emitted from a material when it is exposed to light of a certain frequency. This effect was first observed by Heinrich Hertz in 1887 and later explained by Albert Einstein in 1905 through his theory of quantum mechanics.

2. How does the photoelectric effect work?

The photoelectric effect occurs when a photon of light hits a metal surface and transfers its energy to an electron, causing it to be ejected from the surface. The energy of the photon must be greater than the work function of the metal in order for this to happen.

3. What is the significance of the photoelectric effect?

The photoelectric effect is significant because it provided evidence for the particle nature of light and helped to develop our understanding of quantum mechanics. It also has practical applications, such as in solar panels and photodetectors.

4. How is the photoelectric effect related to the photoelectric equation?

The photoelectric effect is related to the photoelectric equation, which describes the relationship between the frequency of light, the work function of the metal, and the maximum kinetic energy of the emitted electrons. The equation is E = hf - φ, where E is the energy of the electron, h is Planck's constant, f is the frequency of the light, and φ is the work function of the metal.

5. Can the photoelectric effect be observed with all types of light?

No, the photoelectric effect can only be observed with light of a certain frequency, known as the threshold frequency. Light with a frequency below the threshold will not cause the emission of electrons, regardless of its intensity. This supports the particle nature of light, as only photons with enough energy can cause the effect.

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