Critical system in condensed matter physics

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Discussion Overview

The discussion revolves around the concept of critical systems in condensed matter physics, specifically focusing on the transverse Ising model and quantum phase transitions. Participants explore definitions, implications, and characteristics of critical systems, including distinctions between different types of phase transitions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that the transverse Ising model is a critical system due to its phase transition between ferromagnetic and paramagnetic phases when the transverse field is varied.
  • Others clarify that a quantum phase transition occurs at zero temperature and is characterized by tuning parameters, with implications for nonzero temperatures in the quantum critical region.
  • It is noted that the transverse Ising model undergoes a quantum phase transition at a specific point (J=h) and is self-dual.
  • Some participants argue that not all critical systems exhibit symmetry breaking during phase transitions, as seen in topological phases of matter, where distinct states can exist without symmetry breaking.
  • A later reply raises a question about the absence of phase transitions in one-dimensional systems, such as the 1D hopping model, and whether correlation functions can provide significant insights in such cases.

Areas of Agreement / Disagreement

Participants express differing views on the classification of critical systems and the nature of phase transitions, particularly regarding the role of symmetry breaking and the characteristics of topological phases. The discussion remains unresolved on several points, particularly concerning the definitions and implications of critical systems.

Contextual Notes

Participants reference specific models and concepts, such as quantum phase transitions, quantum critical points, and topological insulators, without reaching a consensus on their definitions or implications. There are also mentions of specific conditions under which certain phenomena occur, such as the behavior of the transverse Ising model at T=0.

Who May Find This Useful

This discussion may be of interest to those studying condensed matter physics, particularly in the areas of phase transitions, quantum mechanics, and topological phases of matter.

mimpim
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My question is a little general, and that is how we say that a system is a critical system? for example the transverse Ising model is a critical system? I think the answer is yes, since as we change the transverse field we see that there is a phase transition between ferromagnet and paramagnet phases. Thanks for any comment.
 
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I think you are talking about a system that undergoes a quantum phase transition at a quantum critical point.

A quantum phase transition is defined as a phase transition at zero temperature by tuning some parameter (in the quantum ising model this is the transverse field). However although a QPT is defined as happening at T=0, it still has implications at nonzero temperature in the quantum critical region. This also exists in antiferromagnet transitions. In the cuprate superconductors when you look at a plot of T v doping, the area in between above the quantum critical point is called a strange metal.

You can actually only have an ordered state for the quantum ising model at T=0.
Look at the second edition of quantum phase transitions.
 
radium said:
I think you are talking about a system that undergoes a quantum phase transition at a quantum critical point.

A quantum phase transition is defined as a phase transition at zero temperature by tuning some parameter (in the quantum ising model this is the transverse field). However although a QPT is defined as happening at T=0, it still has implications at nonzero temperature in the quantum critical region. This also exists in antiferromagnet transitions. In the cuprate superconductors when you look at a plot of T v doping, the area in between above the quantum critical point is called a strange metal.

You can actually only have an ordered state for the quantum ising model at T=0.
Look at the second edition of quantum phase transitions.
Thanks for the reply. It gave me lots if useful information. By your answers, it raised some more question for me.
1) by this definition of a critical system that goes through a phase transition by changing a parameter, the transverse Ising model would be a critical system??

2) having an ordered phase is a must for having a phase transition?

Thanks again.
 
1. I wouldn't call these things critical systems, they are systems that undergo quantum phase transition at quantum critical points. The transverse ising model undergoes a quantum phase transition at J=h (it is self dual).

2. No, in topological phases of matter there is no symmetry breaking at the transition but the two states are distinct, by their topology. You can have a transition between a trivial insulator and a Z2 topological insulator just by tuning the spin orbit interaction to get band inversion. You don't break any symmetry going from one to the other but you do go from a topologically trivial system to a nontrivial system, and these two states cannot be smoothly connected.
 
radium said:
1. I wouldn't call these things critical systems, they are systems that undergo quantum phase transition at quantum critical points. The transverse ising model undergoes a quantum phase transition at J=h (it is self dual).

2. No, in topological phases of matter there is no symmetry breaking at the transition but the two states are distinct, by their topology. You can have a transition between a trivial insulator and a Z2 topological insulator just by tuning the spin orbit interaction to get band inversion. You don't break any symmetry going from one to the other but you do go from a topologically trivial system to a nontrivial system, and these two states cannot be smoothly connected.

Thanks again for the explanations. Although I do not know much about topological insulator, but your explanation for (2) was convincing to me. Now I have one more question:
In one dimension (1D) there is no phase transition (for example for the 1D hopping model in a lattice) and if you could calculate the correlation functions, you will get that much physics?
 

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