akhmeteli
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Maaneli said:Once again the configuration space is not part of the definition of 2nd quantization. If you don't understand that, then I'm afraid you are beyond help.
I believe you can see the difference between the following phrases: "the configuration space is a part of the definition of 2nd quantization" and "the configuration space carries a part of the contents of 2nd quantization".
Maaneli said:No, wrong again. The Dirac sea was a part of the 1st quantized Dirac theory well before the development of quantum electrodynamics.
You may call "1st quantized" whatever you want, even SFED. However, the Dirac sea implies the Pauli principle, the Pauli principle implies anticommutation of the relevant operators, and such anticommutation makes a part of the contents of the second quantization. Therefore, the Dirac equation with the Dirac sea carries some of the contents of the second quantization.
Maaneli said:Um, don't you understand that coupling to the Maxwell equations can occur even with the N-particle Dirac equation (in configuration space!)? And don't you understand that the self-field of SFED couples to N-particles as well? Seriously Andy, this is very basic stuff that you should know if you have a PhD in physics and are interested in the foundations of QM.
I do understand that. What I don't understand, is how it is relevant to what I said. And I said that I have in mind application of KSP to the DM equations (or something similar) in (3+1) dimensions (I guess you would call these equations a 1-particle theory). If I am interested in something, that does not mean that nothing else exists in physics, and you are trying to explain to me that there exist other theories, as if I did not know that.
Maaneli, we certainly don’t disagree on what the Fock space is. I repeat, we don’t disagree on that, so there is no need for me to provide my definition of the Fock space, as you suggest in a later post. Just bear with me for a moment, I beg you. I also fully understand that in standard quantum mechanics “for a single particle, you only have ONE Hilbert space, with the corresponding wavefunction evolving in 3+1 dimensions”. BUT! I am talking about what happens AFTER the Kowalski-Steeb procedure is applied to such one-particle theory with wavefunction u(x,t) (in Kowalski’s notation). Please take a short moment for another look at my post #90 (where I give an outline of KSP) or directly at Kowalski’s work. What corresponds to this wavefunction after KSP is the coherent state |u> (or, more exactly, |u,t>, which is not important for the following). Please look at the definition of this state. Up to a certain factor, it’s the vacuum state multiplied by an exponent of a linear combination of creation operators. You can expand this exponent in an infinite series of products of creation operators. What is a vacuum state? It’s a 0-particle state. When you multiply the vacuum state by a creation operator, you get a 1-particle state. When you multiply the vacuum state by a product of n creation operators, you get an n-particle state in the 3n-dimensional configuration space. Thus, the unitary state is a linear combination of k-particle states, where k takes all values from zero to infinity. Therefore, the coherent state lies in the Fock state! Therefore, the 1-particle wavefunctions are embedded into the Fock space. You can repeat ad nauseam that KSP is second quantization, and I’ll repeat ad nauseam that post-KSPT is equivalent to pre-KSPT on the set of solution of the latter. What I want to emphasize is that as a result of KSP, the Fock space naturally arises for the “1-particle” theory. Thus , “to get a Fock space, you” don’t “need to start with more than one particle “, you can just apply KSP to a one-particle wavefunction.Maaneli said:NO! If that's what you think then you clearly don't know what a Fock space is. Let me tell you what it is. The Fock space is the Hilbert space of comprised from the direct sum of tensor products of single-particle Hilbert spaces. For a single particle, you only have ONE Hilbert space, with the corresponding wavefunction evolving in 3+1 dimensions. To get a Fock space, you need to start with more than one particle. That's all there is to it.
As I tried to explain in the previous comment in this post, if you apply KSP to a “one-particle” wavefunction, you get a function in the Fock space. If you then project this function on the 2-particle configuration space (and this projection will not be zero in a general case), you may get an approximation of the singlet state. At least it does not seem obvious that you cannot get such an approximation in this way. I readily admit that I was not taught KSP in the undergraduate QM course.Maaneli said:Well it really should be obvious. I can't believe I am explaining this to you, but if you only quantize the one particle theory, then you simply can't describe (or even approximate) the most basic of entangled states, namely, the singlet-state, which requires TWO wavefunctions corresponding to TWO particles. Again, this is undergraduate QM.