We study the zero-temperature phase diagram of a spin-orbit-coupled Bose-Einstein condensate of spin 1, with equally weighted Rashba and Dresselhaus couplings. Depending on the antiferromagnetic or ferromagnetic nature of the interactions, we find three kinds of striped phases with qualitatively different behaviors in the modulations of the density profiles. Phase transitions to the zero-momentum and the plane-wave phases can be induced in experiments by independently varying the Raman coupling strength and the quadratic Zeeman field. The properties of these transitions are investigated in detail, and the emergence of tricritical points, which are the direct consequence of the spin-dependent interactions, is explicitly discussed
We consider Bose-Einstein condensation of an ideal Bose gas with an equal mixture of ‘Rash...
We consider a spin-1/2 Bose-Einstein condensate with equal Rashba and Dresselhaus spin-orbit couplin...
<p><strong>Figure 3.</strong> Bogoliubov spectrum for Ω/<em>E<sub>r</sub></em> = 2, 4 and 6 for (a)–...
We consider a spin-orbit coupled configuration of spin-1/2 interacting bosons with equal Rashba and ...
We propose a simple model with spin and orbit angular momentum coupling in a spin-1 Bose-Einstein co...
The recent realization of synthetic spin-orbit coupling represents an out-standing achievement in th...
The recent realization of synthetic spin-orbit coupling represents an outstanding achievement in the...
The recent realization of synthetic spin-orbit coupling represents an outstanding achievement in the...
The dissertation explores the effects of synthetic spin-orbit coupling on the behaviour of quantum g...
The internal degrees of freedom provided by ultracold atoms provide a route for realizing higher dim...
Bose-Einstein condensates (BECs) provide an extraordinary system to study many-body quantum effects ...
In spinor Bose-Einstein condensates, spin-changing collisions are a remarkable proxy to coherently r...
The internal degrees of freedom provided by ultracold atoms provide a route for realizing higher dim...
Spin-orbit-coupled bosons can exhibit rich equilibrium phases at low temperature and in the presence...
Abstract. In this paper we investigate the properties of Bose gases with Raman-induced spin-orbit(SO...
We consider Bose-Einstein condensation of an ideal Bose gas with an equal mixture of ‘Rash...
We consider a spin-1/2 Bose-Einstein condensate with equal Rashba and Dresselhaus spin-orbit couplin...
<p><strong>Figure 3.</strong> Bogoliubov spectrum for Ω/<em>E<sub>r</sub></em> = 2, 4 and 6 for (a)–...
We consider a spin-orbit coupled configuration of spin-1/2 interacting bosons with equal Rashba and ...
We propose a simple model with spin and orbit angular momentum coupling in a spin-1 Bose-Einstein co...
The recent realization of synthetic spin-orbit coupling represents an out-standing achievement in th...
The recent realization of synthetic spin-orbit coupling represents an outstanding achievement in the...
The recent realization of synthetic spin-orbit coupling represents an outstanding achievement in the...
The dissertation explores the effects of synthetic spin-orbit coupling on the behaviour of quantum g...
The internal degrees of freedom provided by ultracold atoms provide a route for realizing higher dim...
Bose-Einstein condensates (BECs) provide an extraordinary system to study many-body quantum effects ...
In spinor Bose-Einstein condensates, spin-changing collisions are a remarkable proxy to coherently r...
The internal degrees of freedom provided by ultracold atoms provide a route for realizing higher dim...
Spin-orbit-coupled bosons can exhibit rich equilibrium phases at low temperature and in the presence...
Abstract. In this paper we investigate the properties of Bose gases with Raman-induced spin-orbit(SO...
We consider Bose-Einstein condensation of an ideal Bose gas with an equal mixture of ‘Rash...
We consider a spin-1/2 Bose-Einstein condensate with equal Rashba and Dresselhaus spin-orbit couplin...
<p><strong>Figure 3.</strong> Bogoliubov spectrum for Ω/<em>E<sub>r</sub></em> = 2, 4 and 6 for (a)–...