Quantum Spin Liquid: New State of Matter Explained

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SUMMARY

Quantum spin liquids (SLs) represent a newly discovered state of matter characterized by a spin state that maintains no symmetry breaking at absolute zero temperature. These systems exhibit emergent gauge theories with topological excitations and long-range entanglement, typically found in Mott insulators at half-filling with frustrated interactions. The construction of SLs can be achieved through resonating valence bond states, utilizing the Heisenberg model and Schwinger bosons to describe excitations known as spinons, which behave as fractionalized excitations with spin = 1/2. The mean field theory approach requires careful consideration of constraints to ensure single occupancy, leading to the identification of emergent gauge fields.

PREREQUISITES
  • Understanding of quantum mechanics and many-body physics
  • Familiarity with Mott insulators and frustration in quantum systems
  • Knowledge of gauge theories, particularly Z2 and U(1) theories
  • Experience with mean field theory and the Heisenberg model
NEXT STEPS
  • Study the concept of fractionalization in quantum systems
  • Explore the implications of emergent gauge theories in condensed matter physics
  • Learn about the Heisenberg model and its applications in quantum spin systems
  • Investigate the role of spinons and their interactions in quantum spin liquids
USEFUL FOR

Physicists, condensed matter researchers, and students interested in advanced quantum mechanics and the study of exotic states of matter.

Kevin McHugh
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I just read an article stating physicists have discovered a new state of matter. What is a quantum spin liquid?
 
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A spin liquid is a spin state which breaks no symmetries down to zero temperature. Furthermore it has an emergent gauge theory with topological excitations and long range entanglement. It occurs in Mott insulators at half filling which are "frustrated" i.e. have competing interactions. The gauge theories are usually Z2 or U(1) but only the former is stable in two dimensions.

You can construct a SL from a resonating valence bond state with nearby spins (not always just nearest neighbors) paired in spin singlets (you have all of the possible dimer coverings.) You can construct a mean field theory description from the Heisenberg model using Schwinger bosons (or fermions but this is quite complicated). Excitations above the MF ground state are called spinons which are unpaired spins. In the SL phase they are "deconfined" and can separate as fractionalized excitations with spin =1/2 (this is actually quite similar to the idea of confinement in QCD).

In the MF construction you do not really have an order parameter since you have broken no symmetries. Instead you want to impose single occupancy at all times. Here is where the gauge theory comes in: since mean field theory just imposes the constraint on average, you must find a way to account for this. MF theory can give you states with two or no spins and you need to project out those states. You do this by identifying some emergent gauge field (it comes from a Lagrange multiplier in the Hamiltonian). So the spinons actually interact via this gauge field like charges (there are also monopole like excitations).

Another way to see this is that since you want only one bond coming from each site, you get a "Gauss's law" constraint from considering the RVB state and hence get an emergent gauge theory.

Quantum Field Theory of Many-Body Systems has a whole chapter on SLs.
 
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