Spin liquid states and conductors

Click For Summary

Discussion Overview

The discussion revolves around the nature of spin liquids, particularly whether they can exhibit conducting properties. Participants explore the definitions and characteristics of spin liquids, contrasting them with traditional insulating states, and consider the implications of emergent phenomena such as fractionalization and topological order.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants note that traditional treatments of spin liquids as insulators stem from historical contexts, particularly the resonating valence bond state, which blocks conduction.
  • Others argue that conducting spin liquids are possible, depending on the definitions used, and suggest that concepts like fractionalization and long-range entanglement can describe both insulating and conducting states.
  • A participant expresses skepticism about equating exotic properties of spin liquids, such as emergent gauge structures, with standard definitions of quantum spin liquids (QSLs), particularly in relation to Mott insulators without magnetic ordering.
  • Concerns are raised about the compatibility of spin ordering with the definition of QSLs, with some asserting that a Fermi liquid cannot be a QSL, while a QSL might exhibit Fermi-liquid-like properties.
  • Another participant emphasizes that if a Hamiltonian acts solely on spins, charge conductivity cannot be defined, suggesting that discussions of charge in electronic systems must include electrons or other charge carriers.
  • There is mention of the potential for QSLs to exhibit properties like thermal conductivity, which may motivate further exploration of these states in specific materials, such as triangular lattice organic Mott insulators.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether conducting spin liquids can exist, with multiple competing views presented regarding definitions and characteristics of spin liquids and their relation to conductivity.

Contextual Notes

Definitions of spin liquids and quantum spin liquids are not universally agreed upon, leading to varying interpretations of their properties and implications for conductivity. The discussion highlights the complexity of the relationship between spin ordering, charge conductivity, and emergent phenomena.

mavipranav
Messages
25
Reaction score
0
Hi,

All articles on spin liquids I've seen treat them as insulators. This is understandable in the context in which they were first introduced i.e. the resonating valence bond state in which every electron is singlet-ed with every other, and thus essentially blocking conduction.

Given that that the term spin liquids today, I believe, cover a much broader range of states, why are they still treated as insulators? Put otherwise, why cannot there be conducting spin liquid states?

Thanks,
Mavi
 
Physics news on Phys.org
Depending on what you mean, there is nothing wrong with having a conducting spin liquid. But it demands on what you mean. A Fermi liquid conducts and has no spin ordering so do you consider that a spin liquid? In the context of a purely spin model there is by definition no notion of charge and hence charge conductivity is meaningless. Of course, one can always embed these theories in larger frameworks that include explicit (but gapped) charge degrees of freedom. This leads, for example, to interesting predictions for the ac conductivity.

I would use a more general and less history dependent terminology to describe spin liquids and their more general conducting cousins: ideas like fractionalization and long range entanglement capture nicely the properties of spin liquids while easily generalizing to conducting states. They also make it clear that the "interesting" parts of spin liquids don't really require spin symmetry e.g. fractionalization can coexist with spin ordering.
 
I guess my main problem was, to go into the specifics now, how it might be reasoned that a state with exotic properties like emergent gauge structure or topological order or fractionalisation of charge - as you point out - is equivalent to another standard definition of quantum SL (QSL) i.e. a Mott insulator with no magnetic ordering.

Therefore, I am skeptical that one can have spin ordering and call it a QSL. And no, a Fermi liquid would not be a QSL since such a Hamiltonian acts not on the spins but on the fermions; but the converse, as far as I see, need not hold i.e. a QSL might turn out to have Fermi-liquid like properties.
 
mavipranav said:
I guess my main problem was, to go into the specifics now, how it might be reasoned that a state with exotic properties like emergent gauge structure or topological order or fractionalisation of charge - as you point out - is equivalent to another standard definition of quantum SL (QSL) i.e. a Mott insulator with no magnetic ordering.

One standard answer to this question is the folk theorem that one cannot have a gapped Mott insulator with one electron per unit cell (see Hastings version of LSM theorem for a precise statement, see also the work of Oshikawa http://arxiv.org/abs/cond-mat/0305505 http://arxiv.org/abs/cond-mat/0301338). One can get gapless states by symmetry breaking e.g. AF order (goldstone modes) or a valence bond crystal (degenerate ground states). However, if you rule this out then something "exotic" has to be going on, either topological order or some kind of gapless spin liquid.
Therefore, I am skeptical that one can have spin ordering and call it a QSL. And no, a Fermi liquid would not be a QSL since such a Hamiltonian acts not on the spins but on the fermions; but the converse, as far as I see, need not hold i.e. a QSL might turn out to have Fermi-liquid like properties.

Well, as I said above it depends on your definition. If your definition of QSL is that it isn't spin ordered then sure, but if your definition of QSL is that there are emergent spinons, say, then the two can clearly coexist. Indeed, you can break the spin symmmetry explicitly and not compromise the existence of spinons provided the perturbation is small. Of course their spin quantum number is mixed by the perturbation but one still has emergent fermions.

Also, if you demand a Hamiltonian that acts only on spins then again by definition you cannot have a charge conductivity since there are no charge degrees of freedom. If you want to to talk about charge in an electronic system then you're going to have to at least mention electrons even if some other bosonic mode is carrying the current. Certainly QSLs can have other Fermi liquid-like properties though e.g. thermal conductivity, and this is a major motivation for QSL proposals in the triangular lattice organic mott insulators.
 

Similar threads

  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 0 ·
Replies
0
Views
756
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 5 ·
Replies
5
Views
424
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 16 ·
Replies
16
Views
4K
  • · Replies 46 ·
2
Replies
46
Views
6K
  • · Replies 18 ·
Replies
18
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K