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Lagrangian vs Hamiltonian in QFT vs QM

  1. Feb 11, 2012 #1
    In QFT, Lagrangian is often mentioned. While in QM, it's the Hamiltonian, Is the direct answer because in QFT "position" of particle is focused on and Lagrangian is mostly about position and coordinate while in QM, potential is mostly focus on and Hamiltonian is mostly about potential and coordinate?
     
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  3. Feb 11, 2012 #2

    atyy

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    The Lagrangian is a way to get the Hamiltonian. Sometimes it's easier to incorporate symmetries by using the Lagrangian. The Hamiltonian is still required because it generates "unitary" time evolution. Roughly, unitarity is is what makes probabilities sum up correctly all the time.
     
    Last edited: Feb 11, 2012
  4. Feb 11, 2012 #3
    No;
    The reason people talk about Lagrangians in QFT is because theories are expressed Lorentz-invariantly using the Lagrangian, but not using the Hamiltonian (since the Hamiltonian is an energy which depends on the Lorentz frame).

    In QM, the Hamiltonian is more useful since many problems involve, in some form or other, diagonalizing the Hamiltonian operator (i.e. solving the Schrodinger eqn). This is much more tractable due to fact that most often, the number of degrees of freedom are much fewer than that of QFT.
     
  5. Feb 11, 2012 #4
    So

    Lagrangian = position/velocity
    Hamiltonian = position/momentum, potential

    You mentioned the Lagrangian is a way to get the Hamiltonian, meaning the position/velocity is a way to get the position/momentum and potential? How come?

    Symmetries like U(1)? Why is it earlier in Lagrangian?

    Why, there is no time in Lagrangian?

    Probability can't occur in Lagrangian?
     
  6. Feb 11, 2012 #5
    In short. Lagrangians don't have to involve forces or potential while Hamiltonians do. But I heard you can introduce forces in Lagrangians too, how?


    This is due to the fact that Schrodinger equation solves for potentials and involves energy so Hamiltonian is used and in my original message I mentioned Hamiltonian solves for potential.. so this point is correct.
     
  7. Feb 11, 2012 #6
    Neither the Hamiltonian nor the Lagrangian can directly introduce forces. They have to be added implicitly through the use of a potential; and even then, you would only get conservative forces.

    Neither the Hamiltonian nor the Schrodinger equation solves for potential. The potential is entered into the Hamiltonian manually. The Hamiltonian is part of the Schrodinger equation. You solve that equation.
     
  8. Feb 11, 2012 #7
    Ok I remembered what's one solving in the SE. But what would happen if you use Lagrangian in "diagonalizing the Hamiltonian operator (i.e. solving the Schrodinger eqn)." Is this also possible?
     
  9. Feb 11, 2012 #8
    That's a good question; and the answer is, that is not possible. The Lagrangian is a purely classical object, and does not exist in the realm of quantum mechanics. The Hamiltonian, on the other hand, is an object that appears in both classical mechanics (where it is just a function) and quantum mechanics (which it an operator). However, the Hamiltonian is derivable from the Lagrangian (via a Legendre transform).

    You may then ask, "why are we using the Lagrangian in QFT if we're dealing with a quantum mechanical system?" The answer to that question is because the quantum field theorists are being sneaky: technically, they are using the Hamiltonian which is derived from the Lagrangian they write down, but do not say so. The reason for this is the Hamiltonian is a messy and Lorentz-noninvariant object. Ironically, it also turns out Feynman rules can be read off the Lagrangian much more easily than from the Hamiltonian. But keep in mind that the actual derivation of the Feynman rules must come from the Hamiltonian (unless you use the path-integral approach).
     
  10. Feb 12, 2012 #9

    tom.stoer

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    In QFT one learns how to derive the Lagrangian path integral from the Hamiltonian formulation. Then in most cases one forgets about this derivation and uses directly the Lagrangian PI w/o ever mentioning the Hamiltonian. This is reasonable especially when dealing with Lorentz-covariant scattering calculations where Lorentz covariance is manifest in the Lagrangian whereas it would have to be checked terme by term in a Hamiltonian approach

    Strictly speaking there may be problems with the Lagrangian PI b/c going from the Hamiltonian PI to the Lagrangian PI involves a Gaussian integral which in not be there in general; one theory were this equivalence between Hamiltonian (canonical) and Lagrangian PI is not well understoof ist LQG/SF b/c
    - we do not know the correct (physically, regularized) Hamiltonian yet
    - we do not have a rigorous definiton of the SF model yet
    - and we do not know a rigorous transformation between Hamiltonian and SF model

    In low-energy hadran physics like calculations of properties of bound states like confinement, masses, electromagnetic form factors, ... (even in QCD ) the Hamiltonian is used. Here Lorentz covariance does not play a major role b/c we are looking at one particle (e.g. a proton) at rest and we never want to boost it (we could do that using the Hamiltonian plus other generators of the Lorentz algebra and we would find Lorentz-covariance again, but it would be an awfully difficult calculation).
     
  11. Feb 12, 2012 #10
    I dont understand why physicists tend to "believe" more in hamiltonian than in Langangians. I dont understand neither why they tend to "believe" in canonical quantization than in PI. First of all, from both we can derive the other, so, there is no mathematical obvious choice. And second, there Lagrangian - PI formulation is shorter, clearer (it gives directly the probability amplitude summing up "everything that can happen") and Lorentz invariant. I really think that the "real physics" (meaning the mathematical model that perhaps describes reality without having problems of renormalization, deals with the 4 interactions and so on) is described by an extrapolation of the Lagrangian approach (that is to say, I think that Lagrangian approach is closer to the truth than hamiltonian).
    Why all you people (that studied much more than me) tend to think the other way round?
    Thanks!
     
  12. Feb 12, 2012 #11
    Lagrangian is kinetic energy minus potential energy
    (and the kinetic energy is a function of velocity v and potential energy will typically be a function of position), while

    Hamiltonian is kinetic energy plus potential energy
    (and the Hamiltonian should be expressed as a function of position x and momentum p (rather than position and velocity, as in the Lagrangian)

    Now how come lorentz covariance is manifest in the Lagrangian? I know it is not manifest in the Hamiltonian because time is said to be separate whatever that means.

    Also how come one can derive the Lagrangian from the Hamiltonian and vice versa? For example.

    Lagrangian = 5 - 3 = 2
    Hamiltonain=5 + 3 = 8

    Given 2, how do you figure out its 5 and 3 and not say 100-98?
    Given 8, how do you figure out it's 5 and 3 and not say 6+2?

    Btw.. what is SF in LQG/SF? (I know LQG is Loop Quantum Gravity). Thanks.
    Thanks.
     
  13. Feb 12, 2012 #12

    samalkhaiat

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    This is a mathematical question! and the answer is Legendre transformation. You should have encountered it in your classical mechanics course (if you have taken any). You would be better off spending your time studying physics than asking meaningless questions!
    Sam
     
  14. Feb 12, 2012 #13
    If the Hamiltonian formulation didn't exist before the discovery of the Schroedinger Equation. Would Schroedinger reinvent the Hamiltonian? Or can you formulate the SE without the concept of the Hamiltonian? How?

    Maybe we have a situation now where Superstings Theory haven't discovered the right math or the Hamiltonian equivalent in SE?

    Also it is said the Hamiltonian is an operator. And the solutions of QFT are operators (not observables). So in the context of the Hamiltonian as operators. The solutions of the fields in QFTs are Hamiltonian formulas without any final solutions? I still can't understand what good is to have operators as answer without solving for the values like position or momentum in QFT. Hope someone can address this using the context here. Thanks.
     
  15. Feb 13, 2012 #14

    tom.stoer

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    I don't know if this is true in general. It's my opinion, but I may be wrong.

    If you look at research topics in QM you will mostly find Hamiltonian methods; this could be an indication (but is perhaps no good reason to believe in the Hamiltonian method in QFT)

    I am not so sure about that. When constructing the Lagrangian PI from the Hamiltonian PI you have to integrate out the momenta; this is trivial in standard situations where the momenta always come with p² which results in a Gaussian integral. But in more general situations you can't do the integration! In QM you may find integrals over manifolds with certain symmetries like Sn, SO(n), ... where you have nice geometrical tools available, but w/o these tools you are stuck. So I would say that already in QM it's not always true that you can translate between these two formulations easily.

    As a formal definition - yes.

    But as soon as you want to calculate something that's not always true.

    My impresion is that in the Hamiltonian picture you get a much clearer understanding of the really big problems. In the Lagrangian you can write down many things easily w/o ever thinking about the (mathematical) definiton. With the Hamiltonian things become more complicated - but that's a benefit - at least partially - b/c these problems should alert you that something goes fundamentally wrong (here I mean that you have a fundamental problem, not only a problem with the canonical method).

    But as I said in the beginning, this may be a personal impression based on my experience. I remember some conversations where the Lagrangian approach seemed to be much simpler, but it was not the case that the problems could be solved or did not show up at all; they were simply swept under the carpet.

    there ain’t no such thing as a free lunch ...
     
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