I've been trying to self teach QFT lately. I find that the basic physical idea makes sense, and I can keep up with the mathematical formalism without too much trouble, but I'm having trouble connecting the two.

It is usually said that QFT is necessary because particles can appear and disappear, and so rather than treat a particle as a basic entity as in non-relativistic QM, we instead have a field, and particles are excitations or quanta in that field. In the canonical formalism, the field is a field of operators which creates and destroys particles. For example, if we have a real scalar field $\phi$, then we know that its Fourier components $a_\mathbf{p}$ and $a_\mathbf{p}^\dagger$ act on the vacuum as $a_\mathbf{p}^\dagger |0\rangle = |\mathbf{p}\rangle$. Also, if in the Schrödinger picture $\phi$ is independent of time, that is, $\phi=\phi(\mathbf{x})$, then in the Heisenberg picture we can get time dependence as $\phi(x) = e^{-iHt}\phi(\mathbf{x})e^{iHt} = e^{-ipx}\phi(0)e^{ipx}$.

Looking at the last expression, I don't see how the particles come into play. It seems to me that the current state of the world is "encoded" in the kets, so for example if we have two particles with momentum $\mathbf{p_1}$ and $\mathbf{p_2}$, the state is $|\mathbf{p_1}\ \mathbf{p_2}\rangle$. But it seems that the time evolution of the field depends only on the Hamiltonian and not on (for example) the number of particles. Is this true? If it is, then how does that statement "particles are excitations in a quantum field" translate into the formalism?

Perhaps more simply: is the field any different if we have one particle or if we have two particles?

  • $\begingroup$ The particle number operator should tell you the number of particles at any given spacetime coordinate (or, better, within a finite volume). That's not always a well defined number, though, if I remember correctly. $\endgroup$ – CuriousOne Dec 21 '14 at 15:46
  • $\begingroup$ The time evolution depends on the action of the Hamiltonian on the state, i.e. its energy. The energy of a two-particle state is different from that of a one-particle state, hence the different time-evolutions. $\endgroup$ – glS Dec 21 '14 at 15:48
  • $\begingroup$ Passing away from non-relativistic QM, as you say, to high energy physics isn't where things move from a single wave function $ψ(x⃗,t)$ to n-particle operator tools. You may always rewrite a term $∑_{i≠j}V(|r⃗_i−r⃗_j|)$ of a Hamiltonian describing an n-particle system as $∫∫∫d^3kd^3pd^3q\,V(q⃗ )\,c_{k⃗+q⃗}c_{p⃗−q⃗}c_{p⃗}c_{q⃗}$, where $V(q⃗)$ is the fourier transform of the potential. See e.g. the tight binding model in solid state physics. $\endgroup$ – Nikolaj-K Dec 21 '14 at 19:26

The talk about "particles" being "excitations" is handwavy, and comes about precisely because of the analogy of the usage of Fourier components that you talk about.1

Perhaps more simply, is the field any different if we have one particle or if we have two particles?

"The field" is inaccessible. Some fields aren't even observables (because they may not be (gauge) invariant in and of themselves), and even of these that are, you can only measure the expectation values w.r.t. some states. The statement "particles are excitations" is perhaps most "precise" in the LSZ formalism, where you take some definite-momentum particle-in/out states and obtain that you can calculate

$$\langle p_1,\dots,p_m \vert q_1,\dots,q_n \rangle$$

by looking at some integral whose integrand has $\langle \Omega \rvert T \phi(x_1)\dots\phi(x_m)\phi(y_1)\dots\phi(y_n)\lvert \Omega \rangle$ as a factor, so you could say that this "looks like the field creates the particles".

In QFT, you have to abandon the notion that there is a real value for the field at every point - that would be the classical picture of the field just being the solution of the classical equation of motion. All you can have are expectation values, and the idea that there is some kind of field actually being "excited" is...ill-defined. It isn't clear at all what one would want to say with that. It's just a cute picture that many like, not a mathematically rigorous statement.

Of course, the time evolution will act differently on many-particle states than it will on one-particle states. But these states are states in the Hilbert space of the theory, and only by analogy (since they are created by Fourier components of free fields) identified with "excitations", and analogy that breaks down if we would not consider the asymptotic Fock space but instead the full (but sady, mostly unknown) Hilbert space of the interacting QFT.

1I wrote about this some time ago. The analogy is not very helpful in my view. The mathematics are of the same form as that for an oscillator, but to say that particles are excitations is endowing the concept of field with an ontological weight that is unnecessary, and just tends to confuse people about non-perturbative, interacting QFTs, where it is not helpful at all to think in such terms.

  • $\begingroup$ Maybe one shouldn't talk about particles, at all. It's called QUANTUM mechanics for a reason. If we would be describing particles we would have called it "particle mechanics"... I think that difference throws many off balance, especially when they hear about "particle accelerators" and "particle detectors". I have met older HEP physicists with serious resumes who couldn't let go of the idea that they are juggling little balls... but that breed is thankfully dying out. $\endgroup$ – CuriousOne Dec 21 '14 at 16:10
  • $\begingroup$ @CuriousOne: It would be very good if the distinction between classical particle - blob of matter - and quantum particle - state created by some kind of creation operator, that can be seen to behave somewhat like a classical particle in some contexts - would be made clearer, yes. $\endgroup$ – ACuriousMind Dec 21 '14 at 16:49
  • $\begingroup$ Not an easy educational problem, is it? How do we explain something that is almost completely counterintuitive? $\endgroup$ – CuriousOne Dec 21 '14 at 16:57
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    $\begingroup$ @CuriousOne, you simply teach it without the unnecessary "particle" pictures until it becomes second nature. I cannot think of any time in my life where thinking about 'particles' in QM helped me in any way. I can even go as far and say that it has mostly confused me. But I might be exaggerating... $\endgroup$ – PhotonBoom Dec 21 '14 at 17:06
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    $\begingroup$ @PhotonicBoom: Agreed, the disconnect between science and layman is getting ever harder to bridge. $\endgroup$ – CuriousOne Dec 21 '14 at 18:00

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