By Yoshio Kuramoto, Yusuke Kato

ISBN-10: 0521815983

ISBN-13: 9780521815987

One-dimensional quantum structures exhibit interesting homes past the scope of the mean-field approximation. despite the fact that, the complex arithmetic concerned is a excessive barrier to non-specialists. Written for graduate scholars and researchers new to the sector, this ebook is a self-contained account of the way to derive the unique quasi-particle photo from the precise resolution of versions with inverse-square interparticle interactions. The publication offers readers with an intuitive figuring out of actual dynamical homes by way of unique quasi-particles that are neither bosons nor fermions. strong ideas, reminiscent of the Yangian symmetry within the Sutherland version and its lattice types, are defined. A self-contained account of non-symmetric and symmetric Jack polynomials can also be given. Derivations of dynamics are made more uncomplicated, and are extra concise than within the unique papers, so readers can study the physics of one-dimensional quantum structures in the course of the least difficult version.

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**Additional info for Dynamics of One-Dimensional Quantum Systems: Inverse-Square Interaction Models**

**Example text**

XN ) = Ψ(x1 , . . , xi , . . , xN ). 2) Furthermore, the identity of particles requires the following condition: Ψ(x1 , . . , xi , . . , xj , . . , xN ) = Ψ(x1 , . . , xj , . . , xi , . . 3) which is called the Fock condition. When the coordinates of two particles xi and xj are close, the problem essentially reduces to a two-body problem. 3, the wave function has the asymptotic form |xi − xj | → 0, Ψ → |xi − xj |λ . 4) We consider an N -particle wave function | sin [π (xi − xj ) /L] |λ , ΨB 0 (x1 , .

For both bosons and fermions. 75) can also be regarded as the definition of D for N -particle systems. Through the N -dependence of D, the statistical parameter g is deﬁned by ∆D = −g∆N. 76) In this deﬁnition, g = 0 for bosons and g = 1 for fermions. , Bose or Fermi) statistics, we consider the generalized statistics for any positive value of g. Correlated electron systems provide examples of elementary excitations obeying such statistics; spinon excitations in an antiferromagnetic spin chain obey the statistics g = 1/2, which will be discussed in Chapter 4.

Each region is labeled by α and has the volume V˜α . In the k-space, there is a one-particle state per cell with volume (2π)d /V . Hence in each region α, the number of one-particle states is V /V˜α (2π)d , which is proportional to the volume of the system V . Thus, the exclusion statistics can be deﬁned in each region α. In the case of the Sutherland model, the k-space is replaced by the rapidity space in the above argument. 73) is indeed an example of exclusion statistics. 3 Elementary excitations The low-energy excitation spectra in interacting systems can often be understood in terms of a kind of nearly free particle even when the interaction effect is strong.

### Dynamics of One-Dimensional Quantum Systems: Inverse-Square Interaction Models by Yoshio Kuramoto, Yusuke Kato

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