Positive charge atomic form-factor

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SUMMARY

The positive charge atomic form-factor fnn'(q) describes the positive charge cloud in atoms, particularly for elastic and inelastic scattering processes. This form-factor is determined by atomic wave functions ψn(r) and differs fundamentally from the Hofstadter form-factor. The size of the positive charge cloud can be significantly larger in excited states, such as Rydberg atoms, and is physically analogous to the negative charge atomic form-factor Fnn'(q). The discussion highlights the challenges in experimentally distinguishing between elastic and inelastic scattering processes, emphasizing the importance of fast charged projectiles and large scattering angles.

PREREQUISITES
  • Understanding of atomic wave functions ψn(r)
  • Familiarity with elastic and inelastic scattering processes
  • Knowledge of Rydberg atoms and their properties
  • Basic concepts of atomic form-factors and their significance
NEXT STEPS
  • Research the mathematical derivation of atomic wave functions ψn(r)
  • Study the principles of elastic and inelastic scattering in quantum mechanics
  • Explore the properties and applications of Rydberg atoms in experimental physics
  • Investigate the differences between positive and negative charge atomic form-factors
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Physicists, researchers in atomic and nuclear physics, and students studying quantum mechanics who are interested in atomic scattering phenomena and form-factor analysis.

Have you ever heard/learned of the positive charge atomic formfactor before?

  • Yes, I have.

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Bob_for_short
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IT IS A POLL!

I would like to learn if you've ever heard of the positive charge atomic form-factor before my asking this question. The positive charge atomic form-factor fnn'(q) stands at the nucleus charge Z and describes the positive charge cloud in atoms for elastic scattering at large angles (n→n). It also describes inelastic scattering channels - hitting nucleus by a projectile excites an atom (n→n'). The elastic and inelastic positive charge atomic form-factors are entirely determined with atomic wave functions ψn(r) and they have nothing in common with the Hofstadter form-factor describing the proper nucleus size. The positive "cloud" size may be very big if the initial and the final atomic states ψn(r) are excited and metastable, like in Rydberg atoms. This is just effect of the nucleus motion around the atomic center of inertia. Physically it is of the same nature as the negative (electron) charge atomic form-factor Fnn'(q). The numerical difference is just in the "could" sizes - the negative one is larger (an), the positive is smaller ((me/Mp)an for Hydrogen, for example). Correspondingly the scattering angles where these form-factors work differ essentially - at small and large angles.

The details can be found in my article "Atom as a "dressed" nucleus" in arXiv (http://arxiv.org/abs/0806.2635).

Do not hesitate to leave your answer and thanks for participating in this poll.

Bob_for_short.
 
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You can also leave your opinion on whether the effect of the positive charge smearing in atoms seems to you as realistic as the negative charge smearing or not. Of course, if you have not studied this subject (scattering from atoms, atomic form-factors), leave nothing.

Bob_for_short.
 
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The positive charge cloud in Hydrogen is of the same shape as usual atomic orbitals but scaled down to much shorter distances. See figures for 2p and 3p states. Isn't it beautiful? I added a couple of other pictures.
 

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isnt that just the nuclear shells?
 
granpa said:
isnt that just the nuclear shells?

The term "nuclear" is associated with the strong interactions. It is better to say "a nucleus shell in atom".

Yes, the positive charge cloud is an atomic nucleus shell.

Bob.
 
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Final remark (it is explained in details in "Atom...") concerning observation of these atomic nucleus shells. It is possible in the elastic scattering processes when the initial and the final states of the target atom is the same: ψn(r)→ψn(r). We have to deal with fast charged projectiles whose de Broglie wave-length is smaller than the cloud size. And we have to scatter them at large angles.
In these conditions a fast charged projectile transfers a big momentum to the nucleus so the atom can get easily excited (inelastic processes: ψn(r)→ψn'(r)). In reality it is difficult, without special experimental facility, to distinguish the elastic from inelastic processes. When one observes only the scattered projectiles, all cross section (elastic and inelastic events) are added up experimentally. It is called the inclusive cross section. It is easy to show that the inclusive cross section dσinclusive=∑dσn→n' is reduced quite accurately to the Rutherford cross section, as if the target nucleus were "free" and situated at the atomic center of inertia. This fact explains why the notion of point-like particle finds the "experimental" support. In specially designed experiments one can distinguish the elastic dσn→n from inelastic cross sections and obtain the figures presented above.

The journal version of "Atom..." is available at the Central European Journal of Physics site: http://www.springerlink.com/content/h3414375681x8635/?p=14dbc7f5eda74d6886686dc5b899036d&pi=0

Bob_for_short.
 
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The poll ends up today.
 
Last edited:
The poll had 870 visitors, they left 0 replies "Yes" and 5 replies "No", that is it.
 

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