Exploring Shape Resonance in Air: Oxygen and Nitrogen

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Discussion Overview

The discussion revolves around the concept of shape resonance in air, specifically focusing on the electron impact cross section for nitrogen (N2) and oxygen (O2). Participants explore the implications of shape resonance in the context of ground state nitrogen and its excitation processes, questioning the absence of similar phenomena for electronic excitations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant notes the occurrence of shape resonance in electron impact cross sections and expresses curiosity about its relevance to ground state nitrogen, questioning why it appears in excitation rather than ionization.
  • Another participant suggests that shape resonances arise from the potential energy surface of excited states having local minima, leading to tunneling and dissociation, but expresses confusion about its application to ground state nitrogen.
  • A third participant references a specific paper discussing shape resonance in ground state N2 and seeks clarification on the mechanisms behind this phenomenon and its absence in excited electronic states.
  • One participant explains that the formation of a metastable negative molecular ion occurs during the excitation process, which distinguishes it from ionization, and speculates on the potential for similar effects in excited states.
  • Another participant acknowledges the logic in categorizing the resonance within the excitation spectrum and questions whether negative ions of excited states exist, particularly for the lowest excited state.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and curiosity about the mechanisms of shape resonance, with some agreement on its classification within excitation spectra. However, there remains uncertainty and disagreement regarding the specifics of its occurrence and implications for excited states.

Contextual Notes

Participants reference specific papers and concepts, indicating a reliance on existing literature and suggesting that further exploration of the dynamics involved may be necessary. There are unresolved questions about the behavior of excited states and the conditions under which shape resonance manifests.

Who May Find This Useful

This discussion may be of interest to researchers and students in the fields of plasma physics, molecular physics, and physical chemistry, particularly those focused on electron-molecule interactions and resonance phenomena.

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Greetings. I've been reading papers on plasma kinetics and have come across the term "shape resonance" a few times when describing peaks in electron impact cross section (function of energy). I have seen calculations attempting to explain these for atoms like helium but I'm not sure how close they are to experimental data. However, I am mostly interested in air, good old oxygen and nitrogen. This term comes up with describing ground state nitrogen (N2(X) + e- -> N2(X,v) +e-) and I've found a few papers that discuss this a bit. My crude understanding of this phenomenon is essentially that some kind of metastable ion forms. However, if this is the case than why is this part of the excitation cross section and not the ionization cross section?

On a related note, why do these resonances never show up for electronic excitations? Shouldn't there be similar peaks for the electronic states, N2(A), N2(B), etc.?
 
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Could you be more specific about in which papers you saw shape resonances being discussed?
In my understanding, shape resonances are due to the potential energy surface of some excited state of a molecule having a local (non-global minimum) so that the vibrational states in that minimum decay by tunneling through the barrier (that is, the molecule dissociates).
That's why I don't understand how this terms comes up in the discussion of ground state nitrogen electron scattering from nitrogen molecules. Or do they describe the dynamics of the scattered electron in some inverted Born-Oppenheimer type approximation so that a potential energy surface can be ascribed to the electron?
 
Thank you for the response. An example of what I'm speaking of can be found in Phys. Rev A v56 n.2 (1997) by Sweeney & Shyn. If you don't have access to this journal just message me your email and I can send you a copy. To summarize, the authors are discussing a known shape resonance of the ground state N2 by electron impact. I'm curious to know how this comes about and why excited electronic states do not exhibit this feature at certain electron energies and vibrational levels.
 
I had a look at the article you cited, but I still don't understand your question too well.
The basic process is that of the formation of a metastable negative molecular ion, \mathrm{N_2}+e^- \rightarrow \mathrm{N_2^- }\rightarrow \mathrm{N_2}+e^-.
Obviously this appears in the excitation spectrum and not in the ionization spectrum as the N_2 is only temporarily ionized. Ionization means that something like \mathrm{N_2}+e^- \rightarrow \mathrm{N_2^+}+2e^- takes place.

Similar effects may be possible for excited states N2(A), N2(B) in principle, but to detect them, you would have to start from excited Nitrogen, wouldn't you?
Maybe this article is helpfull:
http://dx.doi.org/10.1103/RevModPhys.45.378
 
Yes, I guess it's very logical that this would fall into the excitation spectrum now that you mention it. I'll take a look at the Schulz article you linked and maybe I'll get a better understanding of this. Before posting this I was assuming that such a region (resonance) in the spectrum only occurred for the ground state since the excited states didn't seem to have similar erratic patterns at certain energy levels, hence me asking why that is true. Perhaps a similar process occurs but it's just far less noticeable. Does the negative ion of an excited state exist? N2(A)-? My guess would be that if this could happen than it would be for the lowest excited state, which is metastable.

N2 + e- -> N2(A)- -> N2(A)+e-
 

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