Where exactly does QFT differ from QM? (in their formalisms)

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Hi.

First off, I'm not sure if this is the right sub to talk about QFT. Apologies if t isn't.

I'm halfway through an introductory QFT course and I still don't get what it is. What is different in its formalism that makes it able to tackle problems that quantum mehanics can't deal with?

From what I know so far I would say that QFT is a generalization of quantum mechanics in which you can "choose" a different equation of evolution, so that QM is a particular case of QFT in which the equation evolution is Schrödinger's equation (or Heisenberg, depending on the picture you choose).

I know this is wrong, though, because another important difference is that the position in space is "demoted" from a operator to a variable, so that it is on the same foot as time. But this makes me wonder many things:

What do we mean exactly when we write Φ(x)?
Are they still wavefunctions or should I think of them as a different concept?
Can these functions be expressed as a scalar product of kets <x|Φ>, as wavefunctions are? If they can what do we substitute the position eigenkets with, since we don't have a position operator anymore?

As you see I am completely lost when I try to see the "big picture". I thought I would find an explicit formalism for QFT somewhere, that is, a presentation of some postulates and the conclusions that follow from them, as there is for quantum mechanics, but every book I've found so far has been unsatisfactory in this regard.

I'd love to hear your thoughts on this.

Thank you for your time.
 

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  • #2
radium
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Are you familiar with second quantization?

QFT comes about when you have an infinite number of degrees of freedom which is required to reconcile QM with special relativity (you can create and destroy particles) but is also natural in condensed matter where you have a very large number of particles and are talking about emergent properties.

\phi(x) is a field with a given amplitude at a point and particles are seen as excitations of the field. You can expand these field in modes of creation and annihilation operators.

And the fields are most definitely operators, you quantize the theory by imposing the canonical commutation relations.
 
  • #3
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QFT takes the field as the fundamental thing that exists rather than the particle and as such already incorporates special relativity into it. This allows creation and annihilation operators and hence the creation and annihilation of particles.
 
  • #4
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Here's the way I think of it - may not be 100% correct.

QM is essentially non-relativistic. When you integrate relativity with QM you're forced to go to QFT.

Schroedinger's equation works as a single-particle equation. The wave function is just a regular function which (in the position representation) gives the probability of finding the particle at that position (by squaring).

When Schroedinger's is made relativistic you get Klein-Gordon (spin 0) or Dirac's equation (spin 1/2). Neither of these equations works right with a single particle. For one thing you get negative energy solutions (which we wind up interpreting as representing the anti-particle). With Klein-Gordon you also fail to get a positive-definite probability density. These facts suggest that we need to abandon the "particle" as a central concept.

Meanwhile experimenters found out that, for one thing, antiparticles do in fact exist; and that particles can be created and destroyed. So they also reinforced the idea that the particle-oriented view was unsatisfactory.

The solution was so-called "second quantization". As I understand it (could be not entirely rigorous) you change the wave function to an operator - actually an infinite bunch of operators - by treating each point of it as an operator. We call that a "field". The particle is demoted to "an excitation of the field" - i.e. a place where the field is particularly intense. Thus there's no longer really a particle, therefore no longer a "position operator". The field itself is a probabilistic representation of the position, just like the wave function it was derived from.

Now it's easy to incorporate multiple particles, creating / destroying particles, and antiparticles, as mere modifications of the field values.

So Φ(x) is, you can informally say, the wavefunction quantized. And Quantum Field Theory comprises the rules for manipulating such objects.

Reviewing your OP I think the above addresses all the questions there, please ask if you think I've missed something.

[EDIT] Of course QFT can be used non-relativistically but it was motivated by relativitistic considerations. In Weinberg *, QFT is brought forward as an unavoidable consequence of the reconciliation of quantum mechanics with special relativity.

"Second quantization" is better termed "field quantization" but the intuitive term is still in use, although deplored by pedants.

In general, for an intuitive understanding, read physics history to see how QFT (or any other topic) was originally motivated.

* Weinberg, S. (2005). The Quantum Theory of Fields 1. Cambridge University Press. ISBN 978-0521670531. page 15.
 
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  • #5
atyy
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As radium says, one approach to second quantization is that it is a way of the exactly rewriting the non-relativistic quantum mechanics of many identical particles as a field theory. (The name second quantization is terrible because historically it was thought of as quantizing the wave function, which is not a very helpful concept, although it is a quick way to generate correct equations.)

So QFT is used in non-relativistic and relativistic physics.
 
  • #6
Demystifier
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QM is a theory of states in the Hilbert space ##{\cal H}_n## with a fixed number ##n## of particles.
QFT is a theory of states in the Hilbert space which is a direct sum ##{\cal H}=\bigoplus_{n=0}^{\infty}{\cal H}_n##.
 
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  • #7
rubi
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The difference between mechanics and field theory is that mechanics is concerned with the motion of point particles (i.e. Newtonian mechanics) and field theory is concerned with the motion of fields (i.e. electrodynamics). The prefix "quantum" just says that we're describing this motion (of point particles or fields respectively) in the framework of quantum physics.

Algebraically, the difference between point particles is encoded in the algebra of observables. For a point particle, you have the following Poisson brackets:
##\{x_i,p_j\}=\delta_{ij}##
For a field theory, the Poisson brackets are given by:
##\{\phi[f],\pi[g]\} = \int_{\mathbb R^3} f(x)g(x)\mathrm d x##
Here, ##f## and ##g## are elements of some suitable test function space and ##\pi## is the conjugate momentum of ##\phi##. In the quantum theory, you replace Poisson brackets ##\{-,-\}## by commutators ##\frac{1}{i\hbar}[-,-]##. The difference between particles and fields is captured completely by these algebraic relations, both in the classical theory and in quantum physics. Everything else stays the same.

QM is a theory of states in the Hilbert space ##{\cal H}_n## with a fixed number ##n## of particles.
QFT is a theory of states in the Hilbert space which is a direct sum ##{\cal H}=\bigoplus_{n=0}^{\infty}{\cal H}_n##.
I wouldn't say this is the difference. First of all, there is a difference between many-particle QM and quantum field theory. The former is concerned with many particles. The latter is concerned with fields. Secondly, Fock space isn't adequate for interacting QFT's anymore due to Haags theorem.
 
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Thank you all.

I think I understand what you all mean, but it still not clicks (maybe it will in time and I am just being impatient). Please tell me if this is correct:

QFT is like quantum mechanics, but the states (for instance ##\vert A \rangle##) represent fields, and the only observables we care about are ##\hat \phi (x)##, which when applied to the ket of a field they give the amplitude ##\hat \phi(x) \vert A \rangle## of the field in that state and in the position ##x##. What we know as particles are certain states of certain fields that have their amplitudes sharply defined in one place.
 
  • #9
A. Neumaier
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Please tell me if this is correct:
No, it is meaningless.

The state of a quantum field system assigns expectation values to all products of its (smeared) fields just as the state of an anharmonic oscillator assigns expectation values to all products of its position and momentum operators. Particles are those states (of an asymptotically free field) where the corresponding number operator (an integral of quadratics in the field) has it as eigenvector with eigenvalue 1.
 
  • #10
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The state of a quantum field system assigns expectation values to all products of its (smeared) fields just as the state of an anharmonic oscillator assigns expectation values to all products of its position and momentum operators.

From this I understand that ##\langle A\vert \phi(x) \vert A\rangle## means the expectation value of the field amplitude in that state and in that position, which is more or less what I (poorly) tried to say. Is that correct?

Particles are those states (of an asymptotically free field) where the corresponding number operator (an integral of quadratics in the field) has it as eigenvector with eigenvalue 1.

I assume the ones with eigenvalue 1 will be one-particle states, and the ones with eigenvalue ##n## will be n-particle states, correct?
 
  • #11
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From the expert point of view QFT may be just a minor gloss on QM: particles => fields, with a few obvious little changes here and there. But for beginners (like you and me), they seem very different. QFT introduces topics such as (non-Hermitian) creation / annihilation operators, Fock states (no good for interactions anymore due to Haags), Feynman diagrams, renormalization, gauge fields, symmetry breaking, Faddeev-Popov ghosts, vacuum state, ... and so forth which you may not have seen in QM.

They can't be addressed in a few posts: that's what your course is for.

But one misunderstanding I can clear up: there are many other field operators besides ϕ! ϕ is a generic term for any field's position operator, the analogue of q or x. There's also a conjugate momentum operator π, analogous to p.

In a given problem there may be many fields considered, most of which have their own ϕ operator. For example in electroweak theory here are some of the types of fields, with their field operators, encountered: lepton spinor fields (Left and Right); W and Z gauge fields - first massless, then given mass by interaction with the isospinor scalar Higgs field; electromagnetic (photon) field; hadron fields; hypercharge field.

I can't imagine how electroweak theory would look in QM, with a particle interpretation.

Perhaps you're getting the main point, but don't think QFT is simple - just change particles to fields and you're done. All the topics mentioned above are probably new, and they're complicated. Your QM knowledge is relevant but QFT is, from the point of view of a student, quite a different beast and you've got your work cut out for you. Good luck!
 
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Perhaps you're getting the main point, but don't think QFT is simple - just change particles to fields and you're done. All the topics mentioned above are probably new, and they're complicated. Your QM knowledge is relevant but QFT is, from the point of view of a student, quite a different beast and you've got your work cut out for you. Good luck!

I know its a different beast, but when I learned QM I was presented with some postulates and was showed their consequences. In QFT I feel like we are using some parts of the formalism of QM and dropping others, but we are never explicitly told which ones. Maybe I'm just overthinking it, I have a tendency for that.

Thanks for your answer.
 
  • #13
A. Neumaier
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From this I understand that ##\langle A\vert \phi(x) \vert A\rangle## means the expectation value of the field amplitude in that state and in that position, which is more or less what I (poorly) tried to say. Is that correct?



I assume the ones with eigenvalue 1 will be one-particle states, and the ones with eigenvalue ##n## will be n-particle states, correct?
yes, yes. But correlations such as ##\langle A\vert \phi(x) \phi(y)\vert A\rangle## are also interesting....
 
  • #14
Avodyne
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I would say that QFT is QM applied to fields. You start with a classical field theory, and then quantize it (using the rules of canonical quantization that apply to any classical mechanical system). This quantized field theory then turns out to describe particles. If the classical field theory is Lorentz invariant, then the particles obey special relativity.

Everything else is details.
 
  • #15
atyy
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I know its a different beast, but when I learned QM I was presented with some postulates and was showed their consequences. In QFT I feel like we are using some parts of the formalism of QM and dropping others, but we are never explicitly told which ones.

All the postulates of QM hold in QFT. In QM, one has Hilbert space, commutation relations, Hamiltonian, observables as Hermitian operators, Born rule and state reduction. All of these hold in QFT.
 
  • #16
dextercioby
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There are so many formulations of QFT and so many formulations of QM, that saying how and where one theory differs from the other is almost impossible. It would be much more useful to learn why the QM (i.e. quantized particle theory) of Dirac, Schrödinger, Heisenberg and von Neumann had to be quickly abandoned in favor of quantized field theory. What exact formalism of QFT you wish to learn (using only path integrals like Bailin and Love do it, or operators like in the classic books) is then your choice (or rather your university lecturer's). The only way to reconcile Dirac's semiclassical theory (electrons quantized, electromagnetic interaction between them beingclassical) with the necessity to quantize the e-m field (first Dirac 1927) was to "invent" a field for the electron, too and from it a Lagrangian and that's how, in time, modern QED was born. Then all particles discovered (positron, neutrino, mesons, etc.) had to follow the old electron and grab a field of their own. So at the level of 1950, it was safe to assume there was only QFT.

This is a must read for any human being studying vigorously physics at university level and hoping to be a physicist someday: http://arxiv.org/abs/hep-th/9702027
 
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  • #17
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This is a must read for any human being studying vigorously physics at university level and hoping to be a physicist someday: http://arxiv.org/abs/hep-th/9702027
Well, maybe not for all physicists, but it is definitely a must read for all theoretical physicists using QFT. It is remarkable how often many particle physicists still argue that certain QFT theory is not appropriate because it is not renormalizable.
 
  • #18
kith
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I know its a different beast, but when I learned QM I was presented with some postulates and was showed their consequences. In QFT I feel like we are using some parts of the formalism of QM and dropping others, but we are never explicitly told which ones.
I made a similar experience when I started to learn QFT. The structure seemed very different from ordinary QM and although everybody said that QFT supersedes it, nobody bothered to relate the two.

Here are some ressources, I found valuable for this (I am actually no expert on QFT and haven't worked through them in detail):
Lecture notes on QFT by David Tong (especially section 2.8.1 "Recovering Quantum Mechanics")
"Student Friendly Quantum Field Theory" by Bob Klauber
"Quantum Field Theory for the Gifted Amateur" by Tom Lancaster and Stephen J. Blundell
 
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  • #19
kith
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What do we mean exactly when we write Φ(x)? Are they still wavefunctions or should I think of them as a different concept?
As others have said, [itex]\phi(\vec x)[/itex] is an operator in QFT. One way to picture it is by its action on the vacuum. The vacuum state is a state with zero particles which is denoted by [itex]|0\rangle[/itex]. If I act on it with the field operator [itex]\phi(\vec x)[/itex], I get a particle localized at location [itex]\vec x[/itex]:
[tex]\phi(\vec x) |0\rangle = |\vec x\rangle[/tex]
So the field operator isn't necessarily an observable but something similar to the creation and annihilation operators you already know from ordinary QM.

What I have written here is by no means rigorous and there are quite a few difficulties. For example, we cannot define a position operator with the usual properties for massless particles like photons. So the very concept of localizing photons isn't well-defined.
 
  • #20
A. Neumaier
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the field operator isn't necessarily an observable but something similar to the creation and annihilation operators you already know from ordinary QM.
In free relativistic QFT, typically ##\phi(x)=a(x)+a^*(x)## (or a constant multiple of it), where ##a(x)## is an annihilation operator distribution in spacetime. (In the classical version, ##a(x)## is called the ''analytic signal'' corresponding to ##\phi(x)##.)

In the interacting case there is no simple relation.
 
  • #21
Every infinite dimensional separable Hilbert space owns a companion non-separable Hilbert space. In the separable Hilbert space a (normal) operator can only have countable eigenspaces. Thus the eigenvalues are rational numbers. In the companion non-separable Hilbert space operators reside that have continuums as eigenspaces. The non-separable Hilbert space can be considered to embed its separable companion. Both types of Hilbert spaces can only cope with number systems that are division rings. Suitable division rings are real numbers, complex numbers and quaternions. Octonions and bi-quaternions are not suitable. The tensor product of two quaternionic Hilbert spaces is a real Hilbert space. Thus quaternionic Fock spaces cannot exist. Dirac invented its bra-ket notation. That notation can be used to link a category of operators to sufficiently continuous functions and in this way a link between multidimensional differentiation and integration methodology can be constructed and the two companion Hilbert spaces can be mapped into each other by this notation method.
In the early days of QM the separable Hilbert space was used. Soon scientist tried to generalize this approach to non-separable Hilbert spaces. Dirac used his Delta function for that purpose. The introduction of the Gelfand triple (rigged Hilbert space) formalized this effort, but that happened several decades later.
The generalized Stokes theorem can be applied to a quaternionic function space. If the boundary is selected at halfway the real axis, then this produces an interesting model that splits the Hilbert spaces in three parts: a history, a static status quo that represents the current state and a future part. Objects that locally obstruct the continuity of the fields must be encapsulated and their contribution must be added separately to the overall solution. These encapsulated regions represent the discrete objects that float over the manifolds that exist in the model.
This view might reveal somewhat more about the relation between QM and QFT. Details can be found in the report that describes the Hilbert Book Test Model.
 
  • #22
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As others have said, [itex]\phi(\vec x)[/itex] is an operator in QFT. One way to picture it is by its action on the vacuum. The vacuum state is a state with zero particles which is denoted by [itex]|0\rangle[/itex]. If I act on it with the field operator [itex]\phi(\vec x)[/itex], I get a particle localized at location [itex]\vec x[/itex]:
[tex]\phi(\vec x) |0\rangle = |\vec x\rangle[/tex]
So the field operator isn't necessarily an observable but something similar to the creation and annihilation operators you already know from ordinary QM.

That's something that irks me quite a bit. How can both that operator and the creation operator create a particle out of the vacuum state? They seem to be different things. Does the first creates a particle with a definite position and the second a particle with a definite momentum?

Also, since particles are actually field excitations, would it be more proper to say that those operators bring the vacuum field state to a field state in which there is a particle in position x or with momentum p?

Thank you all for taking the time to answer my questions, by the way.
 
  • #23
A. Neumaier
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How can both that operator and the creation operator create a particle out of the vacuum state?
This can be seen already for the harmonic oscillator, where ##q=a+a^*## (up to constant factors) replaces the field. In the basis of energy eigenstates, ##a|0\rangle=0##, ##a^*|0\rangle=|1\rangle##, hence ##q|0\rangle=|1\rangle##.
 
  • #24
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The difference between mechanics [i.e. QM] and field theory [i.e. QFT] is that mechanics is concerned with the motion of point particles (i.e. Newtonian mechanics) and field theory is concerned with the motion of fields (i.e. electrodynamics). ... Algebraically, the difference ... is encoded in the algebra of observables. ... The difference between particles and fields is captured completely [my emphasis] by these algebraic relations, both in the classical theory and in quantum physics.

This observation seemed entirely wrong to me, yet I knew it had to be right somehow (why else would rubi say it?) For QFT to depend on only one "axiom" - fields in place of particles - seems superficial to the student. I think I finally figured it out.

From the student's point of view QM is taught as simple and non-relativistic. QFT is presented as though it requires relativity and many new "axioms". (I'll use "axiom" generically to encompass postulates, assumptions, representations, principles.) But the way they're taught is not the way they are. QM actually can be formulated relativistically, and much more generally; and QFT non-relativistically.
All the postulates of QM hold in QFT. In QM, one has Hilbert space, commutation relations, Hamiltonian, observables as Hermitian operators, Born rule and state reduction. All of these hold in QFT.

QM axioms (or, postulates) include 1) math axioms, as in definition of Hilbert Space and 2) physical axioms. Physical axioms are almost all representations, that is, assertions that some mathematical object represents some aspect of the physical world. (Am I using that word correctly?) Thus the squared modulus of the wave function represents chance of finding the particle (position, momentum, etc) there. Particular hermitian operators represent particular observables. And so on.
QFT introduces topics such as (non-Hermitian) creation / annihilation operators, Fock states ..., Feynman diagrams, renormalization, gauge fields, symmetry breaking, Faddeev-Popov ghosts, vacuum state ...

I'm figuring that all these, introduced under the rubric of QFT in the usual curriculum, are equally expressible in QM, i.e. particle view. (If there are exceptions please let me know.) In rubi's view (which I assume is also atyy's, and standard) they belong to general QM. They often require new axioms also.

- Creation / annihilation and the vacuum state: there is a new "axiom" or representation in here somewhere. It has to do with the fact that |0> represents the vacuum, which is not "nothing" but contains the "potentiality" of any particle which is realized by application of appropriate operator.

- Fock states, Feynman diagrams apply in particle view also so the rubi / standard view is, they're part of general QM not QFT per se.

- Renormalization requires some new axiom which states, in effect, "it works".

- Gauge fields: there's some new axiom to the effect that "all QM systems are representable by gauge theories".

- Higgs: This mathematical object "isospinor scalar field" represents the physical Higgs field. My point is, we don't prove it's the Higgs, we assume it, then ultimately show it agrees with experiment.

- Symmetry breaking: This mathematical device represents a physical process that took place around 10^16 degrees, early history of the Big Bang, when Higgs spontaneously went to a random ground state of the "Mexican Hat" distribution.

And so forth.

So, this is why it (incorrectly) seems ridiculous to the student to say that one simple axiom (particles => fields) encapsulates all of QFT! to summarize:

1) All these concepts / mechanisms work in particle view also. So rubi (and I assume all professional physicists?) consider them part of general QM, not QFT.

2) The new concepts one meets in a QFT course do, in fact, require new "axioms" (associated with QM not QFT) but these are never referred to as axioms, often not even stated explicitly. For instance the book doesn't say "Axiom of renormalization: It works" in bold letters, inside a box.

Undoubtedly don't have the right idea 100% but am I in the ballpark?
 
  • #25
A. Neumaier
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am I in the ballpark?
What you call new axioms is usually called new concepts. Each concepts has, so to speak, its own axioms, expressed in its definition. The axioms of QM is only that set of properties that delineate QM from other fields. Similarly for QFT.
 
  • #26
rubi
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- Creation / annihilation and the vacuum state: there is a new "axiom" or representation in here somewhere. It has to do with the fact that |0> represents the vacuum, which is not "nothing" but contains the "potentiality" of any particle which is realized by application of appropriate operator.
Creation/Annihilation operators appear already in non-relativistic QM in the case of the simple quantum harmonic oscillator.

- Fock states, Feynman diagrams apply in particle view also so the rubi / standard view is, they're part of general QM not QFT per se.
Fock space appears in non-relativistic many-particle QM. Feynman diagrams can also be used in the path-integral formulation of non-relativistic QM.

- Renormalization requires some new axiom which states, in effect, "it works".
Renormalization can be used almost everywhere. For example it's heavily used in statistical mechanics. It's not specific to QFT, although QFT uses it a lot. However, in principle, it is also possible to construct QFT's without renormalization (for example free theories and some models in lower dimension).

- Gauge fields: there's some new axiom to the effect that "all QM systems are representable by gauge theories".
Gauge theory isn't a concept of quantum theory. Many classical field theories are already gauge theories, like classical electrodynamics or more generally classical Yang-Mills theory and many more. Of course if you quantize a classical gauge theory, you might get a quantum gauge theory.

- Higgs: This mathematical object "isospinor scalar field" represents the physical Higgs field. My point is, we don't prove it's the Higgs, we assume it, then ultimately show it agrees with experiment.
The Higgs field can also be understood as a classical field and the Higgs mechanism is already present in the classical theory.

- Symmetry breaking: This mathematical device represents a physical process that took place around 10^16 degrees, early history of the Big Bang, when Higgs spontaneously went to a random ground state of the "Mexican Hat" distribution.
Symmetry breaking isn't specific to QFT either. It shows up in many places in physics, for example statistical mechanics.
 
  • #27
It is sensible to spend much more attention to the restrictions that pure mathematics poses. First answer the question why Hilbert spaces are required. Separable Hilbert spaces only feature operators that have countable eigenspaces. Thus the eigenvalues form at the utmost a collection of rational numbers. However, every infinite dimensional separable Hilbert space owns a non-separable companion that features in addition operators that have continuums as eigenspaces. Further, Hilbert spaces can only cope with number systems that are division rings. Only three kinds of suitable number systems exist: real numbers, complex numbers and quaternions. Octonions and bi-quaternions do not fit. The tensor product of two quaternionic Hilbert spaces is a real number based Hilbert space. Thus. Fock spaces cannot use quaternionic Hilbert spaces. They are confined to real or complex number based Hilbert spaces and corresponding eigenspaces!
Depending on their dimension, number systems exist in several versions. For example quaternionic number systems exist in 16 versions that differ in the way that they are ordered. Ordering affects the symmetry. Hilbert spaces can house multiple number systems and multiple versions of these number systems.
 
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  • #28
A. Neumaier
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Renormalization can be used almost everywhere.
even for anharmonic oscillators! The change in frequency due to the anharmonicity is the (mass) renormalization of the ground state.
 
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  • #30
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Thanks A. Neumaier and rubi,

The distinctions between terms like axiom, concept, postulate, representation and so forth are not technically important but can be a real barrier to understanding and communication when misunderstood or mis-applied. Language matters.

For the most part I had no idea these concepts like renormalization had such wide applicability. Many students mistakenly think they're basically part of QFT, since that's where you first meet them. (Although of course classical Maxwell's is a gauge theory). Like the terms mentioned above it's not technically relevant, but it helps to understand where these things really fit in.

fundamentally,

I'm afraid "Hilbert Book Test Model" doesn't sound interesting. But as a mathematician, I'm glad you keep quixotically pushing quaternions! If Hamilton came back he'd be surprised they don't find more use in physics (4 x 4 matrices being preferred). Here's a challenge: invent a notation for quaternions which isn't so clumsy.
 
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  • #31
kith
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How can both that operator and the creation operator create a particle out of the vacuum state? They seem to be different things. Does the first creates a particle with a definite position and the second a particle with a definite momentum?
Yes. In ordinary QM, the position wavefunction can be written as a superposition of momentum eigenstates. Analogously in QFT, the field operator can be written as a sum of operators which create or annihilate a particle with definite momentum. If we act with the field operator on the vacuum, it creates in effect a particle with definite location.
 
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  • #32
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Perhaps like many others, I have been under the (false?) impression that these fields are real In some sense? I am thinking of the buckyball field.
 
  • #33
A. Neumaier
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Perhaps like many others, I have been under the (false?) impression that these fields are real In some sense? I am thinking of the buckyball field.
Why do you mention this? There is no conflict. For every bound state (and hence for buckyballs) there is a corresponding asymptotic field. It is real since one can measure the buckyball density everywhere, though it will be nonzero only where one can actually find the buckyballs. But even a buckyball field operator can be written as the sum of a corresponding creation and annihilation operator.
 
  • #34
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I think what I am struggling with is that an infinite number of different fields are permeating the universe at all times. Are they just mathematical constructs (like virtual particles)?
 
  • #35
A. Neumaier
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I think what I am struggling with is that an infinite number of different fields are permeating the universe at all times. Are they just mathematical constructs (like virtual particles)?
There are a number of basic local fields (those in the standad model and gravity). All other fields are composite fields. In any field theory one can create lots of local composite fields (technically these form the Borchers class of local fields of a theory). In a free QFT, the most general composite local field is given by a linear combination of normally ordered products of local field operators at the same space-time position ##x##. A few of these appear in the Lagrangian density defining a QFT.

In general, composite fields are just mathematical constructs. But some of them have a physical interpretation since they are measurable in an operational sense; the most important ones are the composite fields corresponding to bound states and the associated currents.

A fully defined quantum field theory assigns in each state expectation values of all nonlocal products of the basic fields (technically correlation functions), from which the composite local field expectations (which in the cases mentioned are in principle measurable) are obtained by a limiting procedure (technically through Haag-Ruelle theory). An effective theory concentrates on the few fields and currents relevant at a particular description level for a particular purpose.

So people studying entanglement of buckyballs ignore everything except for the buckyballs. They even dispense with the fields (needed in case the number of buckyballs is not certain) and just look at 1- and 2-particle states where the particle is a buckyball. It would be overkill (and distract from the real physics in buckyball experiments) to represent the buckyballs in terms of quarks and leptons.

For the same reason, engineers concerned with everyday physics ignore the (far too detailed) description of flowing water, say, in terms of quantum fields and represent water instead by a few classical fields, for example energy density, momentum density, and temperature. Each applications therefore has its own effective description, but from a fundamental point of view all these are expectations of certain composite fields.
 

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