A question about graviton self-interactions in QFT

In summary: SUSY, or loops?In summary, the idea is that if one introduces a hypothetical physical principle called "quantum minimal energy", this would remove the perturbations caused by the gravitational interaction from non-SUSY 4D QFT. However, there is no evidence that this is true and the theory is still in development.
  • #1
ensabah6
695
0
Gravity when expressed as QFT suffers from renormalization problems.

From the point of view of the techniques of (four-dimensional) quantum field theory, and as the numerous and heroic efforts to formulate a consistent quantum gravity theory by some very able minds attests, gravitational quantization was, and is still, the reigning champion for bad behavior. There are problems and frustrations stemming from the fact that the gravitational coupling constant has dimensions involving inverse powers of mass, and as a simple consequence, it is plagued by badly behaved (in the sense of perturbation theory) non-linear and violent self-interactions. Gravity, basically, gravitates, which in turn...gravitates...and so on, (i.e., gravity is itself a source of gravity,...,) thus creating a nightmare at all orders of perturbation theory. Also, gravity couples to all energy equally strongly, as per the equivalence principle, so this makes the notion of ever really "switching-off", "cutting-off" or separating, the gravitational interaction from other interactions ambiguous and impossible since, with gravitation, we are dealing with the very structure of space-time itself.​

Suppose one were to introduce as a hypothetical physical principle, the idea of "quantum minimal energy" -- simply put, there is a minimal "quanta" of energy that results in graviton interactions, and below this threshold, there is no graviton interactions. Suppose that one were to conjecture, as a physical principle, the graviton carries too little energy (or for some unknown physical principle, spin-2 particles do not self-interact below a certain threshold)

would this make gravitons perturbation in non-SUSY 4D QFT re-normalizable? While this might seem ad-hoc, if it works, it might be worth researching. Also, there is no technology to explore such incredibly weak effects.

there might not been a need for strings, SUSY, or loops. Just QFT with some additional physical principles, like a cut-off.
 
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  • #2
I am not sure if I get your idea correctly, but I guess that vanishing self-intercation of gravitons below a certain threshold would affect the IR sector only, whereas the divergencies are in the UV.

In addition I do not know how to use this as input. Instead it should be a prediction of the theory (look at QCD: asymptotic freedom = "zero coupling strength in the UV" is a prediction).

Do you know about the "asymptotic safety" research program? It goes back to an idea of Weinberg which is a generalization of asymptotic freedom. It basically says that only a finite number of couplings survive in the UV and that their values remain finite (whereas all other couplings can be neglected). There are some promising results indicating that this could indeed be true in quantum gravity.

Then there is a result of the LQC program which removes singularities like black holes and the big bang entirely. It basically says that gravity coupled to scalar particles becomes repulsive near the Planck scale.

None of these results has been derived rigorously, neither are the fundamental theories widely accepted theoretically or tested experimentally. I mention these results mainly to indicate that there are theories making similar predictions instead of using such an idea as input.
 
  • #3
ensabah6 said:
Gravity when expressed as QFT suffers from renormalization problems.

From the point of view of the techniques of (four-dimensional) quantum field theory, and as the numerous and heroic efforts to formulate a consistent quantum gravity theory by some very able minds attests, gravitational quantization was, and is still, the reigning champion for bad behavior. There are problems and frustrations stemming from the fact that the gravitational coupling constant has dimensions involving inverse powers of mass, and as a simple consequence, it is plagued by badly behaved (in the sense of perturbation theory) non-linear and violent self-interactions. Gravity, basically, gravitates, which in turn...gravitates...and so on, (i.e., gravity is itself a source of gravity,...,) thus creating a nightmare at all orders of perturbation theory. Also, gravity couples to all energy equally strongly, as per the equivalence principle, so this makes the notion of ever really "switching-off", "cutting-off" or separating, the gravitational interaction from other interactions ambiguous and impossible since, with gravitation, we are dealing with the very structure of space-time itself.​

Suppose one were to introduce as a hypothetical physical principle, the idea of "quantum minimal energy" -- simply put, there is a minimal "quanta" of energy that results in graviton interactions, and below this threshold, there is no graviton interactions. Suppose that one were to conjecture, as a physical principle, the graviton carries too little energy (or for some unknown physical principle, spin-2 particles do not self-interact below a certain threshold)

would this make gravitons perturbation in non-SUSY 4D QFT re-normalizable? While this might seem ad-hoc, if it works, it might be worth researching. Also, there is no technology to explore such incredibly weak effects.

there might not been a need for strings, SUSY, or loops. Just QFT with some additional physical principles, like a cut-off.

If I understand correctly you are suggesting a theory where below certain energy scale gravity becomes a linear theory. I guess this may happen if the effective self-interaction couplings vanishes in the IR. This does not happen in GR. However, if there is a theory where this indeed happens you still won't be able to avoid UV divergences. BTW, the asymptotic safety scenario is based on the (non-Gaussian) UV fixed point for the gravitational constant. if this is correct than gravity can be viewed as non-perturbatively renormalizable theory.

P.S. I didn't noticed the previous post. Mine essentially repeats it, sorry
 
  • #4
CHIKO-2010 said:
P.S. I didn't noticed the previous post. Mine essentially repeats it, sorry
No problem.
 
  • #5
As I understand it, the reason QED is renormalizable in QFT, is that while photons carry EM force, photons themselves are uncharged, so it is straightforward to eliminate those infinities.

The reason gravitons is not renormalizable, is that gravitons carry energy and gravitons interact with themselves and everything else, so the infinities in the perturbation series are nonrenormalizable. SUSY attempts to tame these infinities by positing a fermionic SUSY-partner to cancel some of these infinities, string theory attempts to do so via extended interactions and higher dimensions.

What if instead, gravitons do not interact with other gravitons, the way photons in QED do not interact with other photons, b/c gravitons either do not have enough energy, or graviton-spacetime interaction causes them to not interact. Would such gravitons in 4D non-SUSY QFT spin-2 bosons have a perturbation series that is renormalizable?
 
  • #6
ensabah6 said:
As I understand it, the reason QED is renormalizable in QFT, is that while photons carry EM force, photons themselves are uncharged, so it is straightforward to eliminate those infinities.

The reason gravitons is not renormalizable, is that gravitons carry energy and gravitons interact with themselves and everything else, so the infinities in the perturbation series are nonrenormalizable. SUSY attempts to tame these infinities by positing a fermionic SUSY-partner to cancel some of these infinities, string theory attempts to do so via extended interactions and higher dimensions.

What if instead, gravitons do not interact with other gravitons, the way photons in QED do not interact with other photons, b/c gravitons either do not have enough energy, or graviton-spacetime interaction causes them to not interact. Would such gravitons in 4D non-SUSY QFT spin-2 bosons have a perturbation series that is renormalizable?

It is not entirely true that photons do not interact with each other in QED. QED is a nonlinear theory where quantum corrections through the matter loops can induce radiative processes such as e.g., light-by-light scattering. Similar non-linear interactions will be induced if you couple gravitons to matter, in such a way that diff invariance is preserved. Indeed, the linearized gravity coupled to matter is known to be non-renormalizable. Matter loop contributions will be divergent and since the Newton constant has a dimension mass^{-2}, the theory will be non-renormalizable anyway. Diff non-invariant theory of spin-2 field, on the other hand, cannot be a consistent theory. There is no much choice indeed :-)

Renormalizability of QED is essentially due to the fact that the fine structure constant is dimensionless + other stuff (non-anomalous gauge invariance, etc). There are renormalizable non-linear theories also, such as non-Abelian gauge theories: QCD and the electroweak theory. Gluons (QCD cousins of photons) are charged under the color group, but that does not preclude QCD from being a renormalizable theory.
 
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  • #7
CHIKO-2010 said:
It is not entirely true that photons do not interact with each other in QED. QED is a nonlinear theory where quantum corrections through the matter loops can induce radiative processes such as e.g., light-by-light scattering. Similar non-linear interactions will be induced if you couple gravitons to matter, in such a way that diff invariance is preserved. Indeed, the linearized gravity coupled to matter is known to be non-renormalizable. Matter loop contributions will be divergent and since the Newton constant has a dimension mass^{-2}, the theory will be non-renormalizable anyway. Diff non-invariant theory of spin-2 field, on the other hand, cannot be a consistent theory. There is no much choice indeed :-)

Renormalizability of QED is essentially due to the fact that the fine structure constant is dimensionless + other stuff (non-anomalous gauge invariance, etc). There are renormalizable non-linear theories also, such as non-Abelian gauge theories: QCD and the electroweak theory. Gluons (QCD cousins of photons) are charged under the color group, but that does not preclude QCD from being a renormalizable theory.

What about developing a theory of gravity that has a fine structure constant that is dimensionless, but reproduces some of the predictions of GR in the classical limit.
 
  • #8
ensabah6 said:
What about developing a theory of gravity that has a fine structure constant that is dimensionless, but reproduces some of the predictions of GR in the classical limit.

Well, the only consistent theory of that sort known up to now is the string theory
 
  • #9
CHIKO-2010 said:
Well, the only consistent theory of that sort known up to now is the string theory

If QED can have a dimensionless fine structure constant, why can't a gravity be modeled after this, one whose mathematical form exactly duplicates QED?
 
  • #10
ensabah6 said:
If QED can have a dimensionless fine structure constant, why can't a gravity be modeled after this, one whose mathematical form exactly duplicates QED?

No gravity does not duplicate QED. Simply compare Coulomb force with the Newton force. "Charges" for gravity are masses therefore the coupling constant for gravity (the Newton constant) has a dimension mass^{-2} (in natural units).

In the string theory the basic objects are not point-like particles but extended strings, therefore there is inevitably new scale in the theory, the string scale L. The dimensionless string constant than is made up from L and the Newton constant, gs~ L-1GN1/2. this is crude, but I believe correct explanation. The string theory reproduces then Einstein's general relativity for distances > L.
 
  • #11
CHIKO-2010 said:
No gravity does not duplicate QED. Simply compare Coulomb force with the Newton force. "Charges" for gravity are masses therefore the coupling constant for gravity (the Newton constant) has a dimension mass^{-2} (in natural units).

In the string theory the basic objects are not point-like particles but extended strings, therefore there is inevitably new scale in the theory, the string scale L. The dimensionless string constant than is made up from L and the Newton constant, gs~ L-1GN1/2. this is crude, but I believe correct explanation. The string theory reproduces then Einstein's general relativity for distances > L.

the coloumb force is coupled to electric charge. shouldn't gravity really couple to energy rather than mass?
 
  • #12
ensabah6 said:
the coloumb force is coupled to electric charge. shouldn't gravity really couple to energy rather than mass?

Yes, in GR gravity couples to energy and pressure (energy-momentum tensor). I just gave you simpler example of non-relativistic Newton's law, which is obtained from the GR in the corresponding limit. The constant of interactions (the Newton constant) is dimensionfull both in GR as well as in its Newtonian limit. This is the very basics of the theory, I would suggest to consult some textbook, if you are really interested in the subject.
 
  • #13
CHIKO-2010 said:
Yes, in GR gravity couples to energy and pressure (energy-momentum tensor). I just gave you simpler example of non-relativistic Newton's law, which is obtained from the GR in the corresponding limit. The constant of interactions (the Newton constant) is dimensionfull both in GR as well as in its Newtonian limit. This is the very basics of the theory, I would suggest to consult some textbook, if you are really interested in the subject.

ok, but since QED couples to electric charge, why is it "dimensionless"
 
  • #14
ensabah6 said:
ok, but since QED couples to electric charge, why is it "dimensionless"

Dear ensabah6, In the relativistic QFT it is customary to use the units where c=hbar=1, called natural units. In this units the electric charge is dimensionless while Newton's constant has dimension mass-2. The use of these units is also convenient because you can discuss renormalizability of the theory by power counting...Of course you can use whatever units you would like this does not change the conclusion about renormalizability of a given theory.

My sincere suggestion: before attacking such a complicated problems as renormalization of quantum gravitation, it is useful at least to understand very basics of QFT. Sorry, I would not reply anymore to your subsequent post on this matter. Cheers.
 

FAQ: A question about graviton self-interactions in QFT

What is QFT?

QFT stands for Quantum Field Theory. It is a theoretical framework that combines classical field theory with quantum mechanics in order to describe the behavior of subatomic particles and their interactions.

What are gravitons?

Gravitons are hypothetical particles that are predicted by the theory of general relativity. They are thought to be the carriers of the gravitational force, similar to how photons are the carriers of the electromagnetic force.

What are graviton self-interactions?

Graviton self-interactions refer to the interactions between gravitons themselves. In other words, it describes how gravitons interact with each other and affect each other's motion and behavior.

Why is the study of graviton self-interactions important in QFT?

Studying graviton self-interactions is important in QFT because it can help us better understand the behavior of gravity at a quantum level. It can also lead to a more complete understanding of the fundamental forces of nature and potentially help reconcile general relativity with quantum mechanics.

Is there evidence for graviton self-interactions in QFT?

Currently, there is no direct evidence for graviton self-interactions in QFT. However, many physicists believe that they exist based on theoretical predictions and ongoing research in particle physics and cosmology.

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