Wave function is always in abstract space?

In summary: Copenhagen? Many Worlds?In summary, the wave function is always in abstract space in any quantum interpretation be it Copenhagen or Bohmian or Many Worlds because wave function is in many dimensional abstract Hilbert Space. Correct?
  • #1
waterfall
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Wave function is always in abstract space in any quantum interpretation be it Copenhagen or Bohmian or Many Worlds because wave function is in many dimensional abstract Hilbert Space. Correct?

Since the counterpart of Hilbert space in QM is Fock Space in QFT. Then the fields in QFT live in abstract space too. Correct?

This means electron field in QFT live in higher abstract space. But in QED, electromagnetic field live in Fock space too in abstract space, but how come we can detect electromagnetic field? Or is the answer we can't really detect electromagnetic field directly but just the photons when they couple to the electrons in an antenna and vibrate them up and down?

If the answer is we can detect electromagnetic field directly. But electromagnetic field is supposed to live in Fock space in abstract space. So how can we detect or touch things in Fock space when it is supposed to be located in higher abstract space?

Hope someone can clear this up as it sometimes still confused me. Thanks.
 
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  • #2
You pose a lot of hard questions here so let's just start with the first, and I won't attempt an answer to them all. Basically QM is the way it is with complex numbers because it is the only way to have continuous transformations between what are known as pure states - check out:
http://arxiv.org/pdf/quant-ph/0111068v1.pdf

Your other ones require quite a bit of discussion also but just as a start since QFT is a relativistic theory you don't really have an electric field its an electromagnetic field and the quantum of that field is a photon. Electric fields are defined by the force exerted on test particles and that force is the result of an exchange of photons between particles. In this way fields have been reduced to something a little different.

The mathematical spaces they reside in are not the real key - its the physical ideas behind them.

Thanks
Bill
 
  • #3
The wave functions in QFT are not the quantum fields, they still describe the states. The fields are operator valued functions (actually distributions), which are defined on spacetime. So in QFT the fields may be represented by more complicated mathematical obejcts, but they do have as their domain spacetime.

Also it seems that in your questions you make a Freudian distinction between the Hilbert space in QM and Fock space in QFT. They are isomorphic as Hilbert spaces. All the Hilbert spaces, in quantum physics, are isomorphic as abstract Hilbert spaces.
 
  • #4
martinbn said:
The wave functions in QFT are not the quantum fields, they still describe the states. The fields are operator valued functions (actually distributions), which are defined on spacetime. So in QFT the fields may be represented by more complicated mathematical obejcts, but they do have as their domain spacetime.

I see. I was not clear on the distinctions between the wave functions and quantum fields and Fock space. So Fock space is synonym to wave functions when these are put in Hilbert space. And quantum fields are not these.

I heard that electron field are not observable while electromagnetic field are observable.

Just to be clear on something. Although the electron field is not observable, I heard it has components of "grassman numbers". Now if these "grassman numbers" were altered by say the components of real numbers in the electromagnetic field, then there would be corresponding change in the electron particle even though the electron field is non-observable? Something similar to the Aharonov-Effect?




Also it seems that in your questions you make a Freudian distinction between the Hilbert space in QM and Fock space in QFT. They are isomorphic as Hilbert spaces. All the Hilbert spaces, in quantum physics, are isomorphic as abstract Hilbert spaces.
 
  • #5
To talk of "observability", you need to have a theory of observations. This is not a part of the standard quantum theory exposition.

There are several different philosophies here and competing schemes. You must decide in advance what you consider as an "observation" - it must produce a fact, not a "probability distribution of different facts". And this fact should have an appropriate representation in the formal scheme.

By the way: Fock space, or, more generally, a representation space for the algebra of fields, is also a Hilbert space.
 
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  • #6
arkajad said:
To talk of "observability", you need to have a theory of observations. This is not a part of the standard quantum theory exposition.

There are several different philosophies here and competing schemes. You must decide in davance what you consider as an "observation" - it must produce a fact, not a "probability distribution of different facts". And this fact should have an appropriate representation in the formal scheme.

By the way: Fock space, or, more generally, a representation space for the algebra of fields, is also a Hilbert space.

What you talking about. We are all familiar only with interpretations of quantum mechanics, but not interpretations of QFT. We can't imagine what is it like to have a BM or Many Worlds version of QFT. Anyway. When I mentioned wave functions in this thread. I mean the wave functions in quantum fields theory, not nonrelativistic quantum theory of particles (the normal QM everyone knows).
 
  • #7
waterfall said:
We are all familiar only with interpretations of quantum mechanics, but not interpretations of QFT.

"We?" Who? And why are you restricting yourself to BM or Many Worlds?
 
  • #8
arkajad said:
"We?" Who? And why are you restricting yourself to BM or Many Worlds?

I'm not referring to interpretations in QM. But to how are the fields related to the wave functions. But you mentioned it has all to do with interpretations? Anyway. How do you embed Many Worlds in QFT? How do worlds in QFT split?
 
  • #9
waterfall said:
But to how are the fields related to the wave functions
.

You already got the answer: In QFT "wave functions" represent quantum states of the field. Field itself is represented by a space-time net of local algebras (generated by field operators). When the field is a "charged field", then in the field algebra you have a subalgebra of "observables" (very bad name, but used). This subalgebra consists of those field operators that preserve "charge superselection rule" - very important concept.

But you mentioned it has all to do with interpretations? Anyway. How do you embed Many Worlds in QFT? How do worlds in QFT split?

Ask those who split the world. There are other approaches to the measurement problem in QFT that do not rely on scholastic reasonings such as "how many universes can simultaneously dance on the head of a pin?" :smile:
 
  • #10
arkajad said:
.

You already got the answer: In QFT "wave functions" represent quantum states of the field. Field itself is represented by a space-time net of local algebras (generated by field operators). When the field is a "charged field", then in the field algebra you have a subalgebra of "observables" (very bad name, but used). This subalgebra consists of those field operators that preserve "charge superselection rule" - very important concept.

I heard that electron field are not observable while electromagnetic field are observable.

Just to be clear on something. Although the electron field is not observable, I heard it has components of "grassman numbers". Now if these "grassman numbers" were altered by say the components of real numbers in the electromagnetic field, then there would be corresponding change in the electron particle even though the electron field is non-observable? Something similar to the Aharonov-Effect?
 
  • #11
waterfall said:
I heard that electron field are not observable while electromagnetic field are observable.

Just to be clear on something. Although the electron field is not observable, I heard it has components of "grassman numbers". Now if these "grassman numbers" were altered by say the components of real numbers in the electromagnetic field, then there would be corresponding change in the electron particle even though the electron field is non-observable? Something similar to the Aharonov-Effect?

Scratching my head about what you even mean - real numbers altering Grassman Numbers? In QFT everything is a quantum field.

Thanks
Bill
 
  • #12
bhobba said:
Scratching my head about what you even mean - real numbers altering Grassman Numbers? In QFT everything is a quantum field.

Thanks
Bill

Let's take an aquarium as analogy, the fishes and bubbles are the quanta, the water is the electron field. Now if walk toward the aquarium or equivalent to photon field (or electromagnetic field) traveling nearby that touch the aquarium water or electron field, would it affect the fishes or quanta or electrons?
 
  • #13
waterfall said:
I heard that electron field are not observable while electromagnetic field are observable.

Where did you hear that? Electrons can be observed just as well as photons.
 
  • #14
Polyrhythmic said:
Where did you hear that? Electrons can be observed just as well as photons.

In QFT, the electrons are quanta of the electron field. While the photons are quanta of the electromagnetic field. The electron field is unobservable. We can only observe the electrons. In the case of the EM field, we can detect both photons and electromagnetic field.
 
  • #15
waterfall said:
Let's take an aquarium as analogy, the fishes and bubbles are the quanta, the water is the electron field. Now if walk toward the aquarium or equivalent to photon field (or electromagnetic field) traveling nearby that touch the aquarium water or electron field, would it affect the fishes or quanta or electrons?

Again I have zero idea what you are talking about - quanta are not like bubbles and the water is not like an an electron field. These things are are not really describable by classical analogs.

If you are trying to say do photons and electrons interact - yes they do - but the proper description of it is very abstract and mathematical - for a discussion that does not involve it I suggest Feynmans QED Lectures:
http://vega.org.uk/video/subseries/8

Thanks
Bill
 
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  • #16
Electrons are observable. They leave tracks. These track exist whether you look at them or not. Observations of electron positions can be described using quantum field.
 
  • #17
arkajad said:
Electrons are observable. They leave tracks. These track exist whether you look at them or not. Observations of electron positions can be described using quantum field.

Ah... I was thinking that in the electromagnetic field, the antennae can feel its magnetic and electric field but like what Hobba said, in QFT, there is no magnetic or electric fields but just virtual particles that transfer those fields. I was thinking of antennae to receive the electron fields... but they are just electrons... confusing sometimes.. so what's the equivalent of magnetic and electric fields in electron fields and what are the corresponding virtual particles that transfer the corresponding fields? ..
 
  • #18
waterfall said:
In QFT, the electrons are quanta of the electron field. While the photons are quanta of the electromagnetic field. The electron field is unobservable. We can only observe the electrons. In the case of the EM field, we can detect both photons and electromagnetic field.

Not quite - for the EM field all we can detect is photons. An electric field by definition is the force on a test particle exerted by the field, but in QED that is the result of virtual photon exchange from the source of the electric field with the test particle.

Thanks
Bill
 
  • #19
waterfall said:
so what's the equivalent of magnetic and electric fields in electron fields

Electric and magnetic fields are one kind of animals, electron field is another animal. Of course these two kinds of animals leave in a kind of a symbiosis, nevertheless they are two and not just one kind. Ideally nothing prevents you from considering the free electron field. It will approximate certain properties of electrons that are far away one from another, so that their mutual interactions can be neglected.

Antennas and such things - that is quantum electrodynamics and quantum electronics. They have their own methods of describing phenomenologically intensities of the fields.
 
  • #20
bhobba said:
Not quite - for the EM field all we can detect is photons. An electric field by definition is the force on a test particle exerted by the field, but in QED that is the result of virtual photon exchange from the source of the electric field with the test particle.

Thanks
Bill

Ah ok. So in QFT, we can detect photons only. In classical physics. We can detect both electromagnetic wave and electromagnetic field. I thought in QFT, we use the term electromagnetic field to denote an ensemble of photons.. so maybe we must just use "ensemble of photons" but how come I sometimes see the term "Electromagnetic field" used in QFT lessons?
 
  • #21
arkajad said:
Electric and magnetic fields are one kind of animals, electron field is another animal. Of course these two kinds of animals leave in a kind of a symbiosis, nevertheless they are two and not just one kind. Ideally nothing prevents you from considering the free electron field. It will approximate certain properties of electrons that are far away one from another, so that their mutual interactions can be neglected.

Antennas and such things - that is quantum electrodynamics and quantum electronics. They have their own methods of describing phenomenologically intensities of the fields.

So you are saying each quantum field is unique. In electromagnetic field, we have magnetic field and electric fields and their virtual particles. In electron field, we only have electrons. In quark field, we have the gluons and their asymptotic freedom field feature. Is this what you mean each quantum field is unique?
 
  • #22
waterfall said:
In electron field, we only have electrons.

In fact, usually, we also have their antiparticles. So, sometimes it is better to say "elctron-positron field", or "Dirac field".
 
  • #23
waterfall said:
Ah ok. So in QFT, we can detect photons only. In classical physics. We can detect both electromagnetic wave and electromagnetic field. I thought in QFT, we use the term electromagnetic field to denote an ensemble of photons.. so maybe we must just use "ensemble of photons" but how come I sometimes see the term "Electromagnetic field" used in QFT lessons?

It means the quantitised EM field whose quanta are photons (it basically a whole heap of creation and annihilation operators - which a quantum field is) - in QFT the two are synonymous.

Thanks
Bill
 
  • #24
bhobba said:
It means the quantitised EM field whose quanta are photons (it basically a whole heap of creation and annihilation operators - which a quantum field is) - in QFT the two are synonymous.

Thanks
Bill

So in QFT, the analysis is all about particles and virtual particles just like in General Relativity the analysis is all about geometry.

For Faraday, Electric Field has a real field
For QM, Electric Field is in terms of potentials
In QFT, the Electric Field is in terms of virtual particles

You agree all of it?
 
  • #25
waterfall said:
So in QFT, the analysis is all about particles and virtual particles just like in General Relativity the analysis is all about geometry.

For Faraday, Electric Field has a real field
For QM, Electric Field is in terms of potentials
In QFT, the Electric Field is in terms of virtual particles

You agree all of it?

Its not that the analysis is all about particles - its what the math forces on you. When you go through the math you find a field that has been quantized is composed of creation and annihilation which are interpreted as particles ie you take the zero state apply a creation operator to it and you have a particle and so one. The math shows that is what a quantum field it - just a whole heap of creation and annihilation operators applied to the zero state.

Interestingly even bog standard QM (not just QFT) can be formulated that way - which is an interesting formulation because a quantum state can be interpreted as creation and annihilation operators at points in space like a field. A strange sort of field - but maybe not that strange.

Thanks
Bill
 

FAQ: Wave function is always in abstract space?

1. What is a wave function in abstract space?

A wave function in abstract space is a mathematical representation of a quantum system. It describes the probability of finding a particle in a certain state or location. It exists in an abstract mathematical space known as Hilbert space, which has an infinite number of dimensions.

2. Why is the wave function always in abstract space?

The wave function is always in abstract space because it is a mathematical representation of a quantum system, and classical physics concepts such as location and momentum do not apply at the quantum level. The abstract space allows for the description of quantum phenomena that cannot be explained by classical physics.

3. How is the wave function related to the uncertainty principle?

The uncertainty principle states that it is impossible to know both the position and momentum of a particle simultaneously with absolute certainty. The wave function encapsulates this uncertainty by representing the probability of finding a particle in a certain state. The more certain we are about the position of a particle, the less certain we are about its momentum, and vice versa.

4. Can the wave function be observed or measured?

No, the wave function itself is an abstract mathematical concept and cannot be directly observed or measured. However, the effects of the wave function can be observed through experiments and measurements, such as the probability of finding a particle in a certain location or state.

5. How does the wave function change over time?

The wave function evolves over time according to the Schrödinger equation, which describes how the wave function changes in response to the potential energy of the system. As time passes, the wave function spreads out and becomes more diffuse, representing the increasing uncertainty of the particle's position and momentum.

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