7th Workshop on Quantum Chaos and Localisation Phenomena
... a smooth term plus a sum over contributions associated to solutions of the nonlinear Schr¨odinger equation. Our formula applies to bosonic systems with discrete sites, such as the Bose–Hubbard model, in the semiclassical limit as well as in the limit where the number of particles is taken to infinit ...
... a smooth term plus a sum over contributions associated to solutions of the nonlinear Schr¨odinger equation. Our formula applies to bosonic systems with discrete sites, such as the Bose–Hubbard model, in the semiclassical limit as well as in the limit where the number of particles is taken to infinit ...
The Effect of Communication Costs in Solid
... Among these implementations, the solid state systems are perhaps the most intriguing, because of the extensive investment that has been made in semiconductor technology for conventional classical computing, and the potential for scaling to large numbers of qubits. One such scheme, proposed by Kane, ...
... Among these implementations, the solid state systems are perhaps the most intriguing, because of the extensive investment that has been made in semiconductor technology for conventional classical computing, and the potential for scaling to large numbers of qubits. One such scheme, proposed by Kane, ...
Experimental Implementation of Adiabatic Passage between
... Rather than the toric-code model, the first spin-lattice model with topological orders, here we study an alternative exactly solvable spin-lattice model—the Wen-plaquette model [13]. Two different Z2 topological orders exist in this system; their stability depends on the sign of the coupling constan ...
... Rather than the toric-code model, the first spin-lattice model with topological orders, here we study an alternative exactly solvable spin-lattice model—the Wen-plaquette model [13]. Two different Z2 topological orders exist in this system; their stability depends on the sign of the coupling constan ...
The Automorphic Universe
... 2 Kac-Moody Algebras 2.1 Overview of Kac-Moody Algebras . . . . 2.1.1 On Kac-Moody groups: A remark 2.2 Classification of Kac-Moody Algebras . . 2.2.1 Affine Kac-Moody Algebras . . . ...
... 2 Kac-Moody Algebras 2.1 Overview of Kac-Moody Algebras . . . . 2.1.1 On Kac-Moody groups: A remark 2.2 Classification of Kac-Moody Algebras . . 2.2.1 Affine Kac-Moody Algebras . . . ...
Chapter 3 Basic quantum statistical mechanics of spin
... where abc is the completely antisymmetric tensor with xyz = 1. This algebra is familiar as the algebra of generations of rotations (i.e. the components of the angular momentum). Here, the rotation is not in the position of the spins, but rather in its “direction” (in quotes because it is of course ...
... where abc is the completely antisymmetric tensor with xyz = 1. This algebra is familiar as the algebra of generations of rotations (i.e. the components of the angular momentum). Here, the rotation is not in the position of the spins, but rather in its “direction” (in quotes because it is of course ...