We study the Heisenberg antiferromagnetic chain with both dimerization and frustration. The classical ground state has three phases: a Neel phase, a spiral phase and a colinear phase. In each phase, we discuss a non-linear sigma model field theory governing the low energy excitations. We study the theory in the spiral phase in detail using the renormalization group. The field theory, based on an $SO(3)$ matrix-valued field, becomes $SO(3) \times SO(3)$ and Lorentz invariant at long distances where the elementary excitation is analytically known to be a massive spin-$1/2$ doublet. The field theory supports $Z_2 ~$ solitons which lead to a double degeneracy in the spectrum for half-integer spins (when there is no dimerization)
4noWe investigate the ground-state properties of the spin-half J(1)-J(2) Heisenberg chain with a nex...
The linear spin-1/2 Heisenberg antiferromagnet with exchanges J(1) and J(2) between first and second...
We investigate the frustrated two-dimensional S = 1/2 next nearest neighbor anisotropic Heisenberg a...
We study the Heisenberg antiferromagnetic chain with both dimerization and frustration. The classica...
We study the Heisenberg antiferromagnetic chain with both dimerization and frustration. The classica...
The Heisenberg antiferromagnetic spin chain with both dimerization and frustration is studied. The c...
We derive a continuum field theory for the Majumdar-Ghosh model in the large-S limit, where the fiel...
We develop a bosonic mean-field theory to describe the spiral phases of a Heisenberg antiferromagnet...
Using the density-matrix renormalization-group technique, we study the ground-state phase diagram an...
Using the density-matrix renormalization-group technique, we study the ground-state phase diagram an...
9 pages, 8 figuresInternational audienceAiming to describe frustrated quantum magnets with non-magne...
We use a recently developed bosonic mean-field theory to study the ordered ground states of frustrat...
This thesis presents studies of the low energy properties of several frustrated spin-1/2 Heisenberg ...
We present here a nonlinear sigma-model (NL sigmaM) study of a spin-1 antiferromagnetic Heisenberg c...
We report on a detailed investigation of the spin-1 J1−J2−J3 Heisenberg model, a frustrated model wi...
4noWe investigate the ground-state properties of the spin-half J(1)-J(2) Heisenberg chain with a nex...
The linear spin-1/2 Heisenberg antiferromagnet with exchanges J(1) and J(2) between first and second...
We investigate the frustrated two-dimensional S = 1/2 next nearest neighbor anisotropic Heisenberg a...
We study the Heisenberg antiferromagnetic chain with both dimerization and frustration. The classica...
We study the Heisenberg antiferromagnetic chain with both dimerization and frustration. The classica...
The Heisenberg antiferromagnetic spin chain with both dimerization and frustration is studied. The c...
We derive a continuum field theory for the Majumdar-Ghosh model in the large-S limit, where the fiel...
We develop a bosonic mean-field theory to describe the spiral phases of a Heisenberg antiferromagnet...
Using the density-matrix renormalization-group technique, we study the ground-state phase diagram an...
Using the density-matrix renormalization-group technique, we study the ground-state phase diagram an...
9 pages, 8 figuresInternational audienceAiming to describe frustrated quantum magnets with non-magne...
We use a recently developed bosonic mean-field theory to study the ordered ground states of frustrat...
This thesis presents studies of the low energy properties of several frustrated spin-1/2 Heisenberg ...
We present here a nonlinear sigma-model (NL sigmaM) study of a spin-1 antiferromagnetic Heisenberg c...
We report on a detailed investigation of the spin-1 J1−J2−J3 Heisenberg model, a frustrated model wi...
4noWe investigate the ground-state properties of the spin-half J(1)-J(2) Heisenberg chain with a nex...
The linear spin-1/2 Heisenberg antiferromagnet with exchanges J(1) and J(2) between first and second...
We investigate the frustrated two-dimensional S = 1/2 next nearest neighbor anisotropic Heisenberg a...