Legitimacy in visualizing the orbital overlap

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    Orbital Overlap
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Discussion Overview

The discussion revolves around the legitimacy of visualizing orbital overlaps in quantum chemistry, particularly concerning the use of linear combinations of eigenfunctions, such as the dxy, dxz, dyz, dz2, and dx2-y2 orbitals. Participants explore the implications of these representations for chemical bonding and the relationship between real and complex orbitals in various molecular contexts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions the justification for using 'manmade' orbitals if they are not eigenfunctions, despite their success in explaining chemical bonding.
  • Another participant argues that the orbitals in question are indeed linear combinations of eigenfunctions and possess advantages in chemical contexts, such as being real and more localized.
  • A participant seeks clarification on whether real functions are eigenfunctions of relevant operators and if complex functions are less suitable when symmetry is lowered.
  • It is noted that while real functions are not eigenfunctions of Lz, they can still be useful in certain molecular geometries, and complex functions may be preferable in linear molecules.
  • Concerns are raised about the legitimacy of using real orbitals for bonding descriptions, with a suggestion that chemists can often rely on geometric configurations without delving into deeper quantum mechanics.
  • Another participant emphasizes that there is no issue with legitimacy and points out that theoretical chemists typically have a strong grasp of quantum mechanics.

Areas of Agreement / Disagreement

Participants express differing views on the legitimacy and utility of using real versus complex orbitals in chemical bonding. There is no consensus on the best approach, and the discussion remains unresolved regarding the implications of these representations.

Contextual Notes

Participants mention the commutation relations of operators and the relevance of symmetry operations, indicating that the discussion is contingent on specific conditions and assumptions related to the hydrogen atom and molecular environments.

bearcharge
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A chemist is becoming suspicious here:

So, for visual convenience, the so-called dxy, dxz, dyz, dz2, dx2-y2 orbitals are actually linear combination of eigenfunctions. But chemists have been using the geometric feature of these 'manmade' orbitals to make sense the chemical bonding successfully. If they are not eigenfunctions, or 'real' orbitals, how can such success be justified?
 
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This has nothing to do with visual convenience!
The orbitals you are referring to are linear combinations of eigenfunctions of the operators ##L^2## and, at least for the hydrogen atom, of the hamiltonian H. But they are combinations of degenerate eigenfunctions, so they are eigenfunctions themselves and , for the description of an isolated H atom, they are neither superior or inferior to the eigenfunctions of ##L_z##. However, in chemistry they have some definite advantages over the orbitals labeled by the magnetic quantum number m. Namely, they are real and not complex functions and are more localized. I.e. the molecular environment will break in many cases the rotational symmetry around the z axis so that the real valued orbitals which are localized so as to form bonds will remain approximate zeroth order eigenfunctions although their degeneracy is lifted.
 
Thanks for the answer. Just checking if my understanding is correct or not:

1. These real functions are also eigenfunctions of L2, Lz and H (for hydrogen atom) because of the degeneracy.

2. These real functions are good approximations of eigenfunctions when symmetry is lowered/degeneracy is lifted. Is this implying complex functions are not good approximations in this case?

thanks!
 
1. They aren't eigenfunctions of ##L_z##. But there is no good reason why they should, as the hamiltonian does not depend on it.
2. This depends. In linear molecules, it is sometimes better to work with complex functions as the rotational symmetry around the internuclear axis remains (and can be chosen as the z-axis). In most other molecules, the real orbitals have advantages, be it only that you can use float number type instead of complex numbers in computer programs. Generally bonding is better described using e.g. px and py orbitals instead of complex doughnut shaped p+ and p- orbitals.
 
Thanks!

1. Doesn't Lz commute with L2 for hydrogen atom?

2. Can I explain the whole situation to a chemist who does not know quantum physics very well in this way:

The real orbitals we use for describing bonding are actually linear combinations of solved eigenfunctions. They turned out to be appropriate for describing bonding in most situations. So, most of the times, chemists can live happily in a world where they can think about the bonding on the basis of geometric configuration of these real orbitals without worrying out the legitimacy of doing so.

thanks!
 
1. Of course Lz commutes with L2. There are other operators which do so (e.g. trivially Lx or Ly) which do not necessarily commute with Lz. So what is your reason that you insist that a set of degenerate orbitals must be eigenfunctions of Lz? There is no problem with legitimacy.
The hydrogen atom has other symmetry operations which do not even commute with L2 (the Runge Lenz vector). However, they are peculiar to H, too, and thus have also little relevance for chemistry.

2. Beginning physicists have a strange tendency to try to teach chemists how they think how chemistry works. Believe me, at least theoretical chemists have a very good level of quantum mechanics.
 
Thanks for exposing my ignorance on these points and thanks for helping me with a deeper understanding.
 

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