# Hamiltonian Field Theory in Peskin & Schroeder

In Section 2.2 of their QFT textbook, Peskin & Schroeder introduce the Lagrangian and Hamiltonian field theories of a classical scalar field. While defining the action $$S[\phi]$$ and deriving the Euler-Lagrange equation for the classical scalar field $$\phi$$, the classical scalar field $$\phi$$ is considered to be a function of a position $$4$$-vector $$x = (x^0, x^1, x^2, x^3) = (ct, x, y, z)$$.

Then on page no. 16, suddenly they start writing their classical scalar field $$\phi$$ as function of only position vector $$\textbf{x} = (x, y, z)$$ and write Hamiltonian $$H$$ as (Eq. (2.5)) $$H = \int d^3x \left[\pi(\textbf{x}) \dot{\phi}(\textbf{x}) - \mathcal{L}\right].\tag{2.5}$$

After that they again switch back to using the position $$4$$-vector $$x$$ in the discussion of Klein-Gordon equation and write equations where $$\phi$$ is a function of $$x$$; e.g., Eq. (2.8) on page no. 17:

$$H = \int d^3x \, \mathcal{H} = \int d^3x \left[\frac{1}{2}\pi^2 + \frac{1}{2} (\nabla\phi)^2 + \frac{1}{2} m^2\phi^2\right]. \tag{2.8}$$

My Questions

Why is the position $$4$$-vector $$x$$ changed to the position 3-vector $$\textbf{x}$$? What is the motivation for that?

When you transform from the Lagrangian to the Hamiltonian picture, you necessarily must choose a particular foliation of spacetime -- that is, you must single out a particular time direction, and consider surfaces of constant time. One simple way to understand this is that while the Lagrangian is a Lorentz scalar, the Hamiltonian density is the timelike component of the four-momentum density, so its value depends on your choice of space and time axes.

Of course, with that said, there's no reason I can think of that you can't let your classical fields include their time dependence once you pick a time direction. My best guess is that Peskin and Schroeder initially eliminated the time dependence to emphasize that they're considering one particular time slice. They could also have in mind that they're about to quantize their field theory in the Schrodinger picture, where the fields certainly do not depend on time. But they could also just be a bit sloppy here.

• I see. I was probably expecting a line or something there in the textbook to clarify their position. Therefore, your answer certainly helps and thanks a lot for it. Sep 21, 2021 at 21:00
• As per the 2nd paragraph of your answer, in Eq. (2.5), if I assume that fields $\phi$ and $\pi$ are functions of position 4-vector $x$, then $H$ becomes a function of time, because $H = \int d^3 x \mathcal{H}(x) = H(t)$. How would then I interpret this? Sep 24, 2021 at 19:54
• Generically your Hamiltonian can certainly be a function of time -- for instance, if you have a source field $J(x)$. But here, the time dependence is trivial: although $\phi$ and $\pi$ have time dependence, $H$ is a constant of motion and does not evolve. The easiest way to see this is to solve the Klein-Gordon equation for $\phi$ and $\pi$ using a mode expansion, and plug the result back into $H$. Since $H$ is quadratic, it's almost completely identical to the quantum calculation that is performed later in the chapter.
– Zack
Sep 25, 2021 at 8:01

While this is a good book, your question precisely touches on a serious issue: while in equation (2.5) their $$\phi$$ satisfies $$\phi(\mathbf{x}) = \phi(\mathbf{x},t),$$ in equation (2.25) their $$\hat{\phi}$$ satisfies $$\hat{\phi}(\mathbf{x}) \neq \hat{\phi}(\mathbf{x},t)$$ i.e. the $$t$$-dependence completely disappears without a real explanation.

Below equation (2.20) they explicitly say they are setting up the Schrodinger picture, where operators are explicitly time-independent. This is why they are emphasizing the $$\mathbf{x}$$ dependence and not a $$t$$ dependence also.

This might lead one to think the $$t$$ dependence was never there in $$\mathcal{L}$$ and $$\mathcal{H}$$, but it's there in the Klein-Gordon equation and in fact they couldn't derive Klein-Gordon or even use the action formalism without that $$t$$ dependence, so explaining how that $$t$$-dependence goes away is actually important to understand.

They hide the transition from $$t$$ dependence (before (2.25)) to non-$$t$$-dependence (from (2.25) on) both in the notation they use and the 1D Harmonic Oscillator analogy they give after equation (2.20) to argue what the right time-independent fields should look like, obviously the reason for this approach is to emphasize the similarity with Harmonic Oscillators.

That this is all correct is thus again hidden in what they do in section (2.4) showing the Heisenberg picture comes from the time-independent guess they made for what the time-independent Schrodinger picture operator (2.25) should be, even though the Klein-Gordon equation, it's solutions and the action they were using to set it up were all explicitly time-dependent.

So, assuming that the $$t$$ is still there in section 2.2, it explains why the section before equation (2.4) used the $$x = (t,\mathbf{x})$$ notation, and are just emphasizing the $$\mathbf{x}$$ dependence because they want to try to interpret the classical fields as time-independent Schrodinger picture operators (as said below eq. (2.20)).

In (2.25) to (2.28) it's only because they argued by analogy with the 1D Harmonic Oscillator that they can write the general mode expansion of the fields $$\hat{\phi}$$ (and so $$\pi$$) as time-independent. But if one wants to avoid guesses, we should be able to get to (2.25) with the $$t$$ dependence still there, so the $$a_{\mathbf{p}}$$'s are really $$a_{\mathbf{p}}(t)$$'s. There is a very clear jump of logic hidden in this analogy, which is good but can be very confusing.

So if the $$\phi$$'s depend on $$t$$, and so $$x = (t,\mathbf{x})$$, the only way this procedure can be consistent is if the time dependence 'separates' off from the full expansion of the quantum or classical field. If you look between (2.20) and (2.21) they use the time-dependence of the fields on $$t$$ in setting up their 1D Harmonic Oscillator analogy so they are not being consistent with how they deal with $$t$$.

So really, all of this is actually the Heisenberg picture derivation until the guessing starts coming in. Compare to (, Ch. 3) which does a similar derivation (with no analogies) in the Heisenberg picture.

So how would the P&S description go if they didn't guess?

First off, we'd still have to get (2.25) next. We can just write down the general mode expansion of $$\hat{\phi}$$ in (2.25) as the general solution of the Klein-Gordon equation, but with the time-dependence included, i.e. $$\hat{\phi}(x) = \hat{\phi}(\mathbf{x},t)$$. See reference  below, equations (43.3 - 43.11), if you want to see this spelled out in a lot more detail.

We now need to get rid of the $$t$$-dependence in (2.25) to get the Schrodinger picture perspective. If you now look at (2.32), the $$[\hat{H},\hat{a}_{\mathbf{p}}] = ...$$ type relations, or rather their form in terms of exponentials in (2.46), these are the key relations which let us do this. So in this sense it would be good to have done (2.44) to (2.49) next.

Then, using (2.32)/(2.46) it is a simple exercise to re-write the (now time-dependent) $$\hat{\phi}(\mathbf{x},t)$$ in (2.25) as (2.43) which is $$\hat{\phi}(\mathbf{x},t) = e^{\hat{H}t} \hat{\phi}(\mathbf{x})e^{-i \hat{H} t}$$ This, finally, justifies working with the time-independent Schrodinger operators $$\hat{\phi}(\mathbf{x}).$$

Obviously a Schrodinger picture should exist, so they can just assume it exists but they then have to ignore the fact they assumed time-dependence in the Klein-Gordon equation and found it in it's solutions, then just assume they result in a Schrodinger picture operator when quantized, and then just skip the details of the transition by arguing from analogy (as they do after (2.20)) for what the time-independent operators should look like. The justification seems to be that it all works out in section 2.4 since starting from their analogy-based (2.25) you get from this (in (2.43)) a Heisenberg picture which gives back the Klein-Gordon equation.

Without arguing by analogy, only now can we really say the (what they said you're supposed to assume are time-independent, despite using time-dependence again right below them) commutation relations in (2.20) are consistent. We really should have specified they were Heisenberg picture commutators at a fixed time in (2.20) (compare to  eq'n (3.28)). In fact they put "equal-time" in scare-quotes below it after simply stating they were time-independent operators (even though they use time-dependence right below this and say above 2.25 they are talking about the classical Klein-Gordon Hamiltonian which was derived using time-dependent fields, there's simply a big jump there).

So the way to read this is: Section 2.2 has time-dependence (despite the notation) so is the Heisenberg picture; Section 2.3 has no time-dependence (though they use crucially time-dependence in (2.21) justifying their analogy letting them avoid the details of how time dependence is gotten rid of) and they use analogies to argue what the Schrodinger picture should look like; Section 2.4 shows the guess they made in Section 2.3 gives the correct properties one would expect from the Heisenberg-Schrodinger picture transition. They could have just derived the Schrodinger picture by having kept going with the Heisenberg picture perspective and put the guessing after to show it gave the answer one would expect, the price one pays is potentially putting in the kind of derivation given in  and the benefit is supposed to be exploiting one's familiarity with Harmonic Oscillators.

References:

1. Peskin and Schroeder, "Quantum Field Theory", 1st Ed.
2. Srednicki, "Quantum Field Theory", 1st Ed.
3. Woit, "Quantum Theory, Groups and Representations".
• Thanks for taking your time and effort to clarify the subtleties. The answer addresses all of my confusions that I can think of. Also, the summary in the end helps: section 2.2 should be treated time dependent but section 2.3 should not be. Although I am thinking while working through section 2.3, how should I interpret eq. (2.21). Sep 23, 2021 at 14:32
• (2.21) and the one right above it are the Fourier method of solving Klein-Gordon. Plugging it into (2.7) gives (2.21), which is the Harmonic Oscillator equation. We're assuming it's classical so we can just guess it results in a time-independent Harmonic Oscillator Hamiltonian like in QM, but now one for each value of $\mathbf{p}$, so (2.23) is what happens for one $\mathbf{p}$, then we just sum them for all $\mathbf{p}$ as in (2.21) to get (2.25). Further in (2.21) the $e^{i \mathbf{p} \cdot \mathbf{x}}$ is still there, that's why it's complex conjugated in (2.25) via (2.23). Sep 23, 2021 at 14:54
• The above comment is really useful because I can see how the QM ladder op. technique can be applied to solve the quantized theory in QFT. One question though, what does this clause mean: "Further in (2.21) ... there,"? Oct 10, 2021 at 9:53
• Why does the $e^{i \mathbf{p} \cdot \mathbf{x}}$ in the equation above (2.21) get complex conjugated in the second term in (2.25) based on (2.23)? I was trying to argue that it's $\phi(\mathbf{p},t) e^{i \mathbf{p} \cdot \mathbf{x}}$ not just $\phi(\mathbf{p},t)$ that satisfies the SHO equation (2.21), so this is why the $e^{i \mathbf{p} \cdot \mathbf{x}}$ term gets complex conjugated in the second term in (2.25) (giving us the $e^{-i \mathbf{p} \cdot \mathbf{x}}$ term there), looking at it now it's not 100% clear that this makes sense, check it carefully. Oct 11, 2021 at 0:21

The $$t$$-dependence of the various quantities is suppressed in the notation/implicitly implied in the mentioned classical section 2.2 of P&S. E.g. the classical fields $$\phi$$ and $$\pi$$ still depend on the spacetime point $$x=({\bf x},t)$$; not just the position $${\bf x}$$.

The above classical story is closest related to the Heisenberg picture in the corresponding quantum theory. As usual, operators have no time-dependence in the Schrödinger picture, cf. bolbteppa's answer.

• Alright. Thanks, it now makes sense. Sep 21, 2021 at 21:01

The motivation is "by analogous extension" from mechanics with a finite or countable number of degrees of freedom $$H = \sum_a \left(p_a(t) \frac{dq^a(t)}{dt} - L(t,q(t),q'(t))\right)$$ to mechanics with an uncountable number of degrees of freedom $$H = \int \left(π_𝐱(t) \frac{dφ^𝐱(t)}{dt} - 𝔏_𝐱(t,φ^𝐱(t),∂φ^𝐱(t))\right) d^3𝐱$$ to field theory $$H = \int \left(π(𝐱,t) \frac{∂φ}{∂t}(𝐱,t) - 𝔏(𝐱,t,φ(𝐱,t),∂φ(𝐱,t))\right) d^3𝐱.$$

The $$𝐱$$ in $$φ(𝐱,t)$$ is Curried out as $$φ^𝐱(t)$$ and treated as a continuum form of the $$a$$ index in $$q^a$$, and the dependence on $$t$$ is left unmentioned, just as it usually is in the case of mechanics.

The analogy is not an exact fit, since $$𝔏$$ has the extra spatial gradients $$(∇φ)^𝐱(t)$$ in it, not just the time derivatives $$φ_𝐱'(t)$$. There's nothing like them in $$L$$.

• By the way, footnote: the letters $q$ and $φ$ have common origin: the semitic Qoph. And it's still (marginally) present in Greek: Qoppa: Ϙ/ϙ (also Ϟ/ϟ). Nov 13 at 19:33