The following discussion is an archived debate of the proposed deletion of the article below. Please do not modify it. Subsequent comments should be made on the appropriate discussion page (such as the article's talk page or in a deletion review). No further edits should be made to this page.

The result was keep and discuss elsewhere. — CharlotteWebb 17:48, 26 October 2006 (UTC)[reply]

The article's talk page contains under Talk:Quantum theory#expert needed discussion of whether "quantum theory" or "quantum mechanics" is the more general category.

That discussion appears at this time to favor the view that QM is the name for the general theory, which makes a page with this title inappropriate.

David R. Ingham 23:54, 19 October 2006 (UTC)[reply]

There is no such consensus on the talk page. A suggestion on the talk page to merge with quantum mechanics was rejected with only one vote in favor. This AfD is raised in error and should be summarily dismissed. --Michael C. Price talk 05:51, 20 October 2006 (UTC)[reply]

I could have waited longer, but the discussion showed no sign of justifying the page. David R. Ingham 06:09, 20 October 2006 (UTC)[reply]

You should have waited longer. This AfD is in violation of the the guidelines which say that talk page resolution should be sought first. And, as I said, the merge vote went against any change. --Michael C. Price talk 06:28, 20 October 2006 (UTC)[reply]

Looking at a text book for guidance, I find in Bjorken and Drell (1965), chapter 11 (page 2 of the second volume):

Our approach is best illustrated by the electromagnetic field, The potentials A(x) satisfy the Maxwell wave equations and may be considered as describing a dynamical system with an infinite number of degrees of freedom. By this we mean that A(x) at each point of space may be considered an independent generalized coordinate. To make the transition from classical to quantum theory, we must, according to the general principles proclaimed in Chap. 1, elevate coordinates and their conjugate momenta to operators in the Hilbert space of possible physical states and impose quantum conditions upon them. This is the canonical quantization procedure. It is a straightforward extension to field functions, which obey differential wave equations derivable from a lagrangian, of the quantization procedure of non-reLativistic mechanics. When it is done, there emerges a particle interpretation of the electromagnetic field-in the sense of Bohr's principle of complementarity.
If photons emerge in such a natural way from the quantization of the Maxwell field, one is led to ask whether other particles whose existence is observed in nature are also related to force fields by the same quantization procedure. On this basis Yukawa predicted the existence of the meson from knowledge of the existence of nuclear forces. Conversely, it is natural from this point of view to associate with each kind of observed particle in nature a field (x) which satisfies an assumed wave equation. A particle interpretation of the field (x) is then obtained when we carry through the canonical quantization program.

They find nothing revolutionary about this. It is just proceeding to fields, according to the standard methods of quantum mechanics. The first volume is called Relativistic Quantum Mechanics and the second Relativistic Quantum Fields, but there is no suggestion that these are distinct theories. David R. Ingham 01:16, 20 October 2006 (UTC)[reply]

Contrast this to Messiah's text (that might precede this in a curriculum) in which chapters are spent discussing the surprising and fundamental differences between QM and classical physics. David R. Ingham 06:05, 20 October 2006 (UTC)[reply]

This discussion should be taking place on the article's talk page. --Michael C. Price talk 06:29, 20 October 2006 (UTC)[reply]

Messiah makes the point that if electromagnetic fields were not quantized, they would allow measurements to violate the uncertainty principle, so the underlying physics of field theory was already present in early QM. QFT is an approach to making quantum mechanical calculations. David R. Ingham 14:46, 20 October 2006 (UTC)[reply]

And yet quantum field theory and quantum mechanics are taught in separate courses. I wonder why... :-) --Michael C. Price talk 14:52, 20 October 2006 (UTC)[reply]

Hold on, PLEASE READ THIS!

Nobody is coming here to LEARN Quantum Theory. People just want to learn about it! The history of it, or brief history of it. We just want to read and get a general idea of what it is. When I come to the page, and see all of this nonsense about it being deleted, I can't really learn ANYTHING about physics because I don't know if any of it is real or not, when MOST of it is! The person that made this page, never said that what they wrote down and reported here was the end all be all about this subject. Just RELAX! You are putting seeds of doubt in everyones head. That is wrong. Or maybe you are just upset and jealous that he/she got here first, and YOU wanted to do the physics page. Thats just great, "nerd fights". Just relax, and go watch some Star Trek TNG.

I'll watch it with you. ;)

The AfD is clearly erroneous -- I have suggested on the talk page that we vote on whether or not quantum theory should become a pure disambiguation page. --Michael C. Price talk 12:46, 22 October 2006 (UTC)[reply]

The above discussion is preserved as an archive of the debate. Please do not modify it. Subsequent comments should be made on the appropriate discussion page (such as the article's talk page or in a deletion review). No further edits should be made to this page.