<p>The concept of a Tomonaga–Luttinger liquid (TLL) has been established as a fundamental theory for the understanding of 1D quantum systems. Originally formulated as a replacement for the Fermi liquid theory of Landau, which accurately predicts the behaviour of most 3D metals but fails dramatically in 1D, the TLL description applies to an even broader class of 1D systems, including bosons and anyons. After a certain number of theoretical breakthroughs, its descriptive power has now been confirmed experimentally in different experimental platforms. They extend from organic conductors, carbon nanotubes, quantum wires, topological edge states of quantum spin Hall insulators to cold atoms, Josephson junctions, Bose liquids confined within 1D nanocapillaries, and spin chains. In the ground state of such systems, quantum fluctuations become correlated on all length scales, but, counter-intuitively, no long-range order exists. This Review will illustrate the validity of conformal field theory for describing real-world systems, establishing the boundaries for its application, and discuss how the quantum-critical TLL state governs the properties of many-body systems in 1D.</p>

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Platforms for the realization and characterization of Tomonaga–Luttinger liquids

  • Isabelle Bouchoule,
  • Roberta Citro,
  • Timothy Duty,
  • Thierry Giamarchi,
  • Randall G. Hulet,
  • Martin Klanjšek,
  • Edmond Orignac,
  • Bent Weber

摘要

The concept of a Tomonaga–Luttinger liquid (TLL) has been established as a fundamental theory for the understanding of 1D quantum systems. Originally formulated as a replacement for the Fermi liquid theory of Landau, which accurately predicts the behaviour of most 3D metals but fails dramatically in 1D, the TLL description applies to an even broader class of 1D systems, including bosons and anyons. After a certain number of theoretical breakthroughs, its descriptive power has now been confirmed experimentally in different experimental platforms. They extend from organic conductors, carbon nanotubes, quantum wires, topological edge states of quantum spin Hall insulators to cold atoms, Josephson junctions, Bose liquids confined within 1D nanocapillaries, and spin chains. In the ground state of such systems, quantum fluctuations become correlated on all length scales, but, counter-intuitively, no long-range order exists. This Review will illustrate the validity of conformal field theory for describing real-world systems, establishing the boundaries for its application, and discuss how the quantum-critical TLL state governs the properties of many-body systems in 1D.