How Does RG Flow Change Dimensions in Ising Universality Classes?

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SUMMARY

The discussion centers on the relationship between the 2D and 3D Ising universality classes as depicted in figure 1.2 of the paper "http://arxiv.org/abs/0912.3272". It establishes that the renormalization group (RG) flow can indeed change dimensions, particularly when the coupling between neighboring sheets becomes irrelevant. Participants seek further reading on detailed calculations related to this phenomenon, emphasizing the need for deeper understanding of RG flow implications in statistical physics.

PREREQUISITES
  • Understanding of renormalization group (RG) theory
  • Familiarity with Ising models in statistical mechanics
  • Basic knowledge of dimensional analysis in physics
  • Ability to interpret scientific figures and diagrams
NEXT STEPS
  • Read "Renormalization Group and Critical Phenomena" by J. Cardy
  • Explore detailed calculations in "Quantum Field Theory and Statistical Mechanics" by A. Zee
  • Investigate the implications of irrelevant couplings in RG flow
  • Study the relationship between dimensionality and critical behavior in phase transitions
USEFUL FOR

Physicists, particularly those specializing in statistical mechanics, theoretical physicists studying phase transitions, and researchers interested in the mathematical foundations of renormalization group theory.

atyy
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In http://arxiv.org/abs/0912.3272 , figure 1.2 says that the 2D and 3D Ising universality classes are related by a renormalization flow. How can the RG flow change dimension? Is there anything I could read that does the calculation in more detail?
 
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atyy said:
In http://arxiv.org/abs/0912.3272 , figure 1.2 says that the 2D and 3D Ising universality classes are related by a renormalization flow. How can the RG flow change dimension? Is there anything I could read that does the calculation in more detail?

Maybe if the coupling between neighbouring sheets becomes irrelevant?
 

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