Question about Radiationless De-Excitation

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Discussion Overview

The discussion revolves around the concept of radiationless de-excitation in atomic physics, specifically focusing on the mechanisms of energy transitions between electron energy levels, the differences between emission and absorption spectra, and the conditions under which these processes occur. The scope includes theoretical explanations and conceptual clarifications related to atomic structure and spectral analysis.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes radiationless de-excitation as a process where an electron can lose energy without emitting a photon, but questions why this occurs at certain excitation levels and not at ground levels.
  • Another participant clarifies that the quantized nature of electron states means energy changes require interaction with the electromagnetic field or other means, such as collisions, and emphasizes that electrons cannot lose energy "by themselves."
  • A different participant critiques the use of "orbits" to describe atomic structure, suggesting that this model is outdated and does not apply to atoms other than hydrogen, proposing that photon exchange is the primary means of energy transfer in atomic interactions.
  • One participant reflects on their initial question about the differences between emission and absorption spectra, noting that the emission spectrum contains a wider range of frequencies than the absorption spectrum.
  • Another participant elaborates on the differences between the two spectra, mentioning that absorption spectra show characteristic dips due to re-radiation in different directions and that some frequencies can cause permanent internal changes.
  • A participant expresses uncertainty about an external explanation regarding emission and absorption spectra, suggesting that emission spectra arise from high-energy conditions while absorption spectra occur in colder regions where most atoms are in the ground state.
  • Concerns are raised about the phrasing of "random states" in the context of emission spectra, with a suggestion that the term "more possible states" would be more accurate, as energy states are discrete rather than blurred.

Areas of Agreement / Disagreement

Participants express differing views on the mechanisms of radiationless de-excitation, the appropriateness of the "orbits" model, and the nature of emission and absorption spectra. There is no consensus on these topics, and multiple competing perspectives remain throughout the discussion.

Contextual Notes

Some limitations include the dependence on specific definitions of energy states and the unresolved nature of the mechanisms behind radiationless de-excitation. The discussion also reflects varying interpretations of spectral phenomena without reaching a definitive conclusion.

Kavi
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Hello,

I understand that an electron in an atom can:

1. Absorb any amount of energy from a photon and become excited
2. It may move to a higher energy orbit or remain in the current orbit
3. To move to a lower energy orbit, it must release excess energy so it is at the ground level of the current orbit (Radiationless Deexcitation)
4. Moving to a lower orbit, it will release a photon with properties dependent on the structure of the atom.

If the above is correct, I want to ask,

The mechanism for 3. above is Radiationless Deexcitation. I wanted to know more about this.

Specifically, why does this happen at other excitation energy levels but not at ground energy levels for any given orbit?
 
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I don't understand what
Kavi said:
it must release excess energy so it is at the ground level of the current orbit
means.

The state of the electron is quantized, meaning that it can only exists in certain discrete states of energy. To change state, it must receive or give away energy, which is most often through interaction with the electromagnetic field (absorption/emission of photons). But it can also exchange energy through other means, such as collisions. This is how you could have radiation less de-excitation. But the electron cannot lose energy this way "by itself."
 
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@Kavi
Describing the structure of an atom in terms of “orbits” is very old fashioned. It fails because there are many other energy states of all but the Hydrogen atom where that simple mechanical model doesn’t work.

In any case, any interaction between charged particles is best described in terms of a photon exchange. Afaik there’s no other magic way for energy to get around in the low energy world of atoms and molecules
 
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Thanks guys, the responses helped, and I did some more researching and found what I was looking for.

Basically, what I meant to ask for was the difference between the emission spectrum and the absorption spectrum, but I didnt know to frame the question in those terms.

If I understand this correctly now, then there is some little difference between the two spectrums and they are not pure inversions of each other, the emission spectrum contains wider frequencies than those of the absorption spectrum.
 
Kavi said:
the difference between the emission spectrum and the absorption spectrum,
You were asking about 'point 3'. if the energy is all internal then there will be no emission or absorption.
Kavi said:
the emission spectrum contains wider frequencies than those of the absorption spectrum.
When we observe absorption spectra, the radiation is often re-radiated but in other directions. hence the apparent dip at certain characteristic frequencies. Other frequencies can cause internal changes which may be permanent or semi permanent.
 
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sophiecentaur said:
You were asking about 'point 3'. if the energy is all internal then there will be no emission or absorption.

When we observe absorption spectra, the radiation is often re-radiated but in other directions. hence the apparent dip at certain characteristic frequencies. Other frequencies can cause internal changes which may be permanent or semi permanent.

Hi, thanks for that. I found the below explanation on another site but I am not sure if it is exactly correct?

In the emission spectrum, the electrons in the energy levels usually start at random energy levels and so there is more of a variety of wavelengths that could possibly be emitted.

Whereas in the absorption spectrum, there are a few lines missing because most electrons start from ground state, meaning that there are less options of energies that a photon can be emitted at.

https://physics.stackexchange.com/q...ion-spectrum-than-on-the-emission-spectr?rq=1
 
Kavi said:
Hi, thanks for that. I found the below explanation on another site but I am not sure if it is exactly correct?
https://physics.stackexchange.com/q...ion-spectrum-than-on-the-emission-spectr?rq=1
This is more of an observation than an explanation. I would put it this way:

Emission spectra are generated in regions where there are 'high energy' conditions, with fast electrons around (for instance). Temperatures can be high and so there will be significant numbers of atoms in higher states than the ground state or even ionised.

"Random states" would only occur in very extreme conditions of pressure and temperatures where the energy states are spread (line broadening - look up Pauli Exclusion Principle). But I don't think this applies here: states are not Random or blurred but discrete. The phrasing should be "more possible states".

Absorption spectra are seen in cold regions of gas where most atoms are in the ground state. But the absorbed (star) light will be re-emitted in other directions over the whole sphere. The spectrum of this light will tend to be a single line.
 

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