Abstract
The generalized (1+1)-D non-linear Schrodinger (NLS) theory with particular integrable boundary conditions is considered. More precisely, two distinct types of boundary conditions, known as soliton preserving (SP) and soliton non-preserving (SNP), are implemented into the classical $gl_N$ NLS model. Based on this choice of boundaries the relevant conserved quantities are computed and the corresponding equations of motion are derived. A suitable quantum lattice version of the boundary generalized NLS model is also investigated. The first non-trivial local integral of motion is explicitly computed, and the spectrum and Bethe Ansatz equations are derived for the soliton non-preserving boundary conditions.
Original language | English |
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Pages (from-to) | 465–492 |
Number of pages | 28 |
Journal | Nuclear Physics B |
Volume | 790 |
Issue number | 3 |
DOIs | |
Publication status | Published - 21 Feb 2008 |
Keywords
- hep-th
- math-ph
- math.MP
- nlin.SI