Relativistic Quantum Mechanics

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Discussion Overview

The discussion revolves around the application of the Klein-Gordon equations to the simple harmonic oscillator and subsequently to the hydrogen atom. Participants explore the potential corrections and precision improvements that might arise from this approach, while also considering the historical context and existing theories such as the Dirac equation and quantum electrodynamics (QED).

Discussion Character

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

Main Points Raised

  • One participant proposes applying the Klein-Gordon equations to the simple harmonic oscillator and then to the hydrogen atom to achieve more precise results.
  • Another participant questions the validity of this approach, suggesting that the Dirac equation already provides accurate solutions for the hydrogen atom.
  • A participant mentions that the Schrödinger equation was historically derived from the Klein-Gordon equation, but later found to be more effective for hydrogen.
  • Concerns are raised about the differences in solutions between the simple harmonic oscillator and the hydrogen atom, particularly regarding the presence of Hermite polynomials and angular momentum considerations.
  • Discussion includes the potential corrections that might arise from solving the relativistic equations compared to non-relativistic ones.
  • One participant notes that the minimally coupled Klein-Gordon equation for the hydrogen atom yields results similar to the Dirac case, but with some differences in terms that appear in the expansions.
  • Another participant highlights the historical context of the equations and the necessity of quantum field theory for addressing certain difficulties in the relativistic treatment of particles.

Areas of Agreement / Disagreement

Participants express differing views on the effectiveness and implications of using the Klein-Gordon equations for the hydrogen atom. There is no consensus on whether this approach would yield more accurate results than existing methods, and multiple competing perspectives remain throughout the discussion.

Contextual Notes

Participants note the limitations of the Klein-Gordon and Dirac equations in accounting for electromagnetic interactions without the full framework of quantum field theory. The discussion also touches on the historical development of these equations and their applications, indicating that some assumptions and dependencies on definitions may not be fully resolved.

ziad1985
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I got an idea today , what different thing will we get if we applied the Klein-Gordon Equations to The Simple harmonic oscillator?
then take it to the hydrogen atome and see how much corrections will we get??
wouldn't we get more precise results?or it just can't be done?did someone already did this work or what?
 
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How on Earth would doing a KG harmonic oscillator and then "taking it" (I have no idea what you mean by this) to hydrogen atom give anything more accurate than what's already gotten via solving the Dirac eq?
 
I don't remember how exactly to do it , but you can derive hydrogen energy and other stuff from The simple harmonic oscillator.
anyway forget that for a second,I'm still learning Non-relativistic Quantum mechanics , but it was an idea crossed my mind.
so dirac eq involves solving the relativistic wave eq of the hydrogen atom?
 
You mean using a relativistic field equation to predict the bound states etc. of hydrogen, instead of the Schrödinger equation? You'd have to use QED, the Klein-Gordon and free-Dirac fields don't account for electromagnetic interactions, well the latter can if you apply minimal coupling but without quantum field theory one can only account for first order interactions. If you do apply QED to hydrogen you get things like the lamb-shift: very slight shifts in the emission spectra of hydrogen from the non-relativistic prediction (i.e. Schrödinger).
 
hmmm , but what kind of corrections will i get solving the Relativistic eq ?
 
i mean in comparision to non-relativistic , and what is the order of precision?
 
ziad,

Historically, Schrödinger actually wrote the Klein-Gordon equation down first as a putative wave equation for the electron. As the story goes, he solved the Klein-Gordon equation for hydrogen and found that the results did not agree with the observed spectra. His second attempt was the Schrödinger equation we all know. Furthermore, as has been mentioned above, it is the Dirac equation that describes the electron, and in the context of relativistic wave mechanics, it is this equation that should be used to compute corrections. There are well known difficulties with this approach that must eventually be dealt with by using the powerful methods of quantum field theory. In the end, the full radiative corrections of QED are evident as in the Lamb shift, the anomalous magnetic moment, and so on.
 
Last edited:
ziad1985 said:
I don't remember how exactly to do it , but you can derive hydrogen energy and other stuff from The simple harmonic oscillator.
anyway forget that for a second,

I can't, because this would be VERY strange.

Look at the solution to the SHO - you get Hermite polynomials. Now look at the solution to the H atom. Do you see any Hermite polynomials anywhere? What about the angular momentum part in SHO? Any sign of it?

And what about the fact that when you do SHO problems, you put the center of the potential at the origin, and you have a symmetric potential around that point. You have both - and + displacement of the oscillator. Do you have such a solution in H atom? is "-r" (not a vector) for the radial part a physical solution in spherical coord?

Zz.
 
Physics Monkey: i see thank you a lot.
but this bring me to another question what are the real uses of the klein-gordon equations , where do they benefit the most,other then using them for relativistic moving particles?

ZapperZ:I honestly don't remember where i saw that , I think maybe it was in a book i was reading, it was an approch to get the energy of the atome , but maybe I'm mixing some other thing up or the writer was a whacko , which the latter seem more convincing because i still don't understand how did he do it.
 
  • #10
ZapperZ said:
I can't, because this would be VERY strange.

Look at the solution to the SHO - you get Hermite polynomials. Now look at the solution to the H atom. Do you see any Hermite polynomials anywhere? What about the angular momentum part in SHO? Any sign of it?

And what about the fact that when you do SHO problems, you put the center of the potential at the origin, and you have a symmetric potential around that point. You have both - and + displacement of the oscillator. Do you have such a solution in H atom? is "-r" (not a vector) for the radial part a physical solution in spherical coord?

Zz.
Actually, as far as I remember, there is an equivalency between the Schroedinger 3d Coulomb and 4d oscillator problems, it arises from the dynamical symmetry of 3d Coulomb problem discovered by Fock. To demonstrate this equivalency one writes 3d Coulomb in momentum space and introduces stereographic coordinates, or something like that. Sorry, I am very vague here, and I cannot give a reference to online resources, but this reference seems to be relevant, although I haven't read the article itself: http://prola.aps.org/abstract/PRA/v22/i2/p333_1
I agree, however, that it would be very strange to see this in an entry level course
 
  • #11
If you solve the minimally coupled KG equation for the H atom, you get a formula containing a sq.root (just like in the Dirac case, see Greiner's book on "Relativistic Wave equations") and if you do power series expansion of that sqrt, you'll get some terms which can be found in the Dirac case (like the original Balmer formula, the relativistic correction and the B coupled to L part), but some will not occur: namely B coupled to S and L coupled to S. WHY ? Well, in CFT KG is the equation of motion for a spin 0 particle, while in the Dirac case: C,P,T and all possible combinations invariance + spin 1/2 determine the form of the equation.

As for H atom vs 3D harmonic oscillator, well the wave function contains the same angular part (L_z L^2 and H are a c.s.c.o. for both systems) and the radial one is a confluent hypergeometric function which degenerates to two different types of orthogonal polynomials: Laguerre & Hermite.

Daniel.
 

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