Renormalization and scale dependence

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SUMMARY

The discussion centers on the concept of scale dependence in quantum field theory (QFT), as introduced by Wilson's work in the 1970s. Participants explore how scale dependence manifests through various methods, including perturbative cutoff and lattice techniques, and its implications for effective theories. The conversation highlights the relationship between scale dependence and universality, particularly in the context of Kadanoff's block spin picture and critical exponents in phase transitions. Additionally, the dialogue touches on the limitations of using high-energy collisions to uncover true field theories and suggests alternative approaches, such as examining low-energy deviations.

PREREQUISITES
  • Quantum Field Theory (QFT) fundamentals
  • Renormalization techniques in physics
  • Kadanoff's block spin picture
  • Understanding of universality and critical phenomena
NEXT STEPS
  • Study Wilson's renormalization group approach in depth
  • Explore Kadanoff's block spin transformations and their applications
  • Investigate the implications of Haag's theorem in QFT
  • Research the relationship between scale dependence and symmetry breaking in classical theories
USEFUL FOR

Physicists, particularly theoretical physicists and researchers in quantum field theory, as well as students seeking to understand the implications of scale dependence and universality in physical systems.

TrickyDicky
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Since Wilson work in the 70s, the renormalization technique in QFT is physically justified with the concept of scale dependence(scale anomaly) of the parameters.
This apparently is akin to a universal version of the characteristic length usually applied to specific physical systems to define their scale.

Can anybody explain how is this scale dependence introduced(independently of the specific procedure:perturbative cutoff, dimensional, lattice...)? Where does it come from?

Does the Haag's theorem imply that this scale dependence technique is not even related to the QFT lagrangian?
 
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A circle seen from far away may look like a point, so a point is an effective theory of a circle. But if one looks under the microscope, one will see that it is a circle. So the theory one uses - point or circle - depends on how closely or finely one looks. Scale dependence in quantum field theory is an analgous idea. If we probe the system using low energies and long wavelengths, then we will be looking at the system more coarsely. If we probe the system using high energies and short wavelengths, then we will be looking at the system more finely. Just like the microscope, as we change how finely we look, the theory changes in a way which is manifest in the scale dependence.

Of course, one can get much more dramatic changes than scale dependence, like uncovering new degrees of freedom.

The basic idea is described by Kadanoff's block spin picture https://www.amazon.com/dp/0521804426/?tag=pfamazon01-20
 
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This is actually a very deep question.

Murray Gell-Mann gave a talk on it - its actually tied up with beauty in physics and math:


Its this scale dependence that causes the same things to pop up over and over.

Thanks
Bill
 
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atyy said:
A circle seen from far away may look like a point, so a point is an effective theory of a circle. But if one looks under the microscope, one will see that it is a circle. So the theory one uses - point or circle - depends on how closely or finely one looks. Scale dependence in quantum field theory is an analgous idea. If we probe the system using low energies and long wavelengths, then we will be looking at the system more coarsely. If we probe the system using high energies and short wavelengths, then we will be looking at the system more finely. Just like the microscope, as we change how finely we look, the theory changes in a way which is manifest in the scale dependence.

Yes, this is the usual metaphor. It basically amounts to trivially admitting we are stuck with the coarse view of the point and the circle scapes us so far. IOW that we don't have the right picture that Gell-Mann refers to in the talk linked by Bill.

The problem I see with this metaphor is that people take it too literally in the sense that theyseem to infer from it that the only way to advance towards the true (not just effective) field theory is by smashing matter with ever higher energies.

bhobba said:
This is actually a very deep question.

Murray Gell-Mann gave a talk on it - its actually tied up with beauty in physics and math:


Its this scale dependence that causes the same things to pop up over and over.

Thanks
Bill

I remember that talk, it just touches upon the scale dependence issue, it is more concerned with the highly related concept of universality(when he talks about the similarity of the onion layers) that can be found in the renormalization group both in high energy physics and in condensed matter physics, i.e.: sameness of critical exponents in Kadanoff's second order phase transitions terms.

Probably both the scaling and the approximate self-similarity are sides of the same coin.
 
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TrickyDicky said:
Yes, this is the usual metaphor. It basically amounts to trivially admitting we are stuck with the coarse view of the point and the circle scapes us so far. IOW that we don't have the right picture that Gell-Mann refers to in the talk linked by Bill.

The problem I see with this metaphor is that people take it too literally in the sense that theyseem to infer from it that the only way to advance towards the true (not just effective) field theory is by smashing matter with ever higher energies.

I think there are two other ideas out there. The first is to look for deviations from the present theory at low energy (eg. the discussion between Gross and Strassler reported by Motl http://motls.blogspot.com/2014/03/gross-vs-strassler-gross-is-right.html). The second is still to smash things at higher energy, but to realize that it may be too expensive for us, but maybe we can use cosmological observations (eg. BICEP2, if it pans out).

Anyway, yes, I believe we agree on scaling. Scaling is just one a manifestation of different effective theories at different scales. Universality has to do with fixed points occurring as one performs scaling or renormalization flow.
 
atyy said:
I think there are two other ideas out there. The first is to look for deviations from the present theory at low energy (eg. the discussion between Gross and Strassler reported by Motl http://motls.blogspot.com/2014/03/gross-vs-strassler-gross-is-right.html).
I would side with Strassler there.

Anyway, yes, I believe we agree on scaling. Scaling is just one a manifestation of different effective theories at different scales. Universality has to do with fixed points occurring as one performs scaling or renormalization flow.
I think it is interesting to contrast this scale dependence associated with quantum effects against the scale invariance of the classical theories. More commonly discussed in terms of(spontaneous) breaking of symmetries.
There is room to think that rather than symmetry beaking we might be facing the failure of approximate but not exact symmetries to account for the quantum effects.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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