Spin-dependent Transport of Interacting Electrons in Mesoscopic
... and AlGaAs [4]. With present techniques atomically sharp interfaces between the different materials can be achieved. Because of the different band gaps of the distinct materials a band bending occurs close to the interface forming a sharp quantum well in the y-direction perpendicular to the plane of ...
... and AlGaAs [4]. With present techniques atomically sharp interfaces between the different materials can be achieved. Because of the different band gaps of the distinct materials a band bending occurs close to the interface forming a sharp quantum well in the y-direction perpendicular to the plane of ...
Two Provers in Isolation
... Commitments”, at QIP ’06, The 9th Workshop on Quantum Information Processing, January 16-20, 2006, Paris. Supported in part by CIFAR, NSERC, MITACS, QuantumWorks and FQRNT’s INTRIQ ...
... Commitments”, at QIP ’06, The 9th Workshop on Quantum Information Processing, January 16-20, 2006, Paris. Supported in part by CIFAR, NSERC, MITACS, QuantumWorks and FQRNT’s INTRIQ ...
vortices - University of Toronto Physics
... In this simple picture the core is like a string, in which the superfluid density goes to zero at the origin - the core has a finite diameter, because the singularity in the phase cannot persist in bulk superfluid. In He-4 this diameter is very small (only about 1 Angstrom!), but in other superfluid ...
... In this simple picture the core is like a string, in which the superfluid density goes to zero at the origin - the core has a finite diameter, because the singularity in the phase cannot persist in bulk superfluid. In He-4 this diameter is very small (only about 1 Angstrom!), but in other superfluid ...
bYTEBoss introduction
... • No definitive answer to this question yet! • In 1967 A. Sacharov formulated a set of general conditions that any such mechanism has to meet 1) You need a process that violates the baryon number B: (Baryon number of matter=1, of anti-matter = -1) 2) Both C and CP symmetries should be violated ...
... • No definitive answer to this question yet! • In 1967 A. Sacharov formulated a set of general conditions that any such mechanism has to meet 1) You need a process that violates the baryon number B: (Baryon number of matter=1, of anti-matter = -1) 2) Both C and CP symmetries should be violated ...
Terahertz driven intraband dynamics of excitons in nanorods Fredrik Sy
... Quantum dots and nanorods are becoming increasingly important structures due to their potential applications that range from photovoltaic devices to medicine. The majority of the research on carrier dynamics in these structures has been in the optical regime, with little work performed at Terahertz ...
... Quantum dots and nanorods are becoming increasingly important structures due to their potential applications that range from photovoltaic devices to medicine. The majority of the research on carrier dynamics in these structures has been in the optical regime, with little work performed at Terahertz ...
Scattering theory - Theory of Condensed Matter
... a loosely bound pair, whose size can become comparable to or even larger than the average distance between particles. A Bose-Einstein condensate of these fragile pairs is called a “BCS-state”, after Bardeen, Cooper and Schrieffer. This is what occurs in superconductors, in which current flows withou ...
... a loosely bound pair, whose size can become comparable to or even larger than the average distance between particles. A Bose-Einstein condensate of these fragile pairs is called a “BCS-state”, after Bardeen, Cooper and Schrieffer. This is what occurs in superconductors, in which current flows withou ...
The electronic Hamiltonian in an electromagnetic field
... where ρ (r, t) and J (r, t) are the charge and current densities, respectively, of the particles in the system, whereas 0 and µ0 are the electric constant (the permittivity of vacuum) and the magnetic constant (the permeability of vacuum), respectively. As we shall see later, the electric and magne ...
... where ρ (r, t) and J (r, t) are the charge and current densities, respectively, of the particles in the system, whereas 0 and µ0 are the electric constant (the permittivity of vacuum) and the magnetic constant (the permeability of vacuum), respectively. As we shall see later, the electric and magne ...
Plasma Electrodynamics and Applications—A. Bers, A. K. Ram
... collisional transport phenomena in plasmas confined by a strong, external magnetic field, and on the single-fluid magneto-hydrodynamic (MHD) description of low-frequency dynamics.3,4 For a plasma in a strong magnetic field, so-called gyro-viscous terms, that are independent of collisions, were disco ...
... collisional transport phenomena in plasmas confined by a strong, external magnetic field, and on the single-fluid magneto-hydrodynamic (MHD) description of low-frequency dynamics.3,4 For a plasma in a strong magnetic field, so-called gyro-viscous terms, that are independent of collisions, were disco ...
Calculation of the nucleon axial charge in lattice QCD
... by examining our recent computation of the nucleon axial charge. ...
... by examining our recent computation of the nucleon axial charge. ...
109, 105302 (2012)
... A new research direction in low dimensional condensed matter physics that has attracted much recent attention is the study of two-dimensional (2D) topological quantum states of matter (e.g., fractional quantum Hall effects, chiral p-wave superfluids or superconductors, etc.) that support exotic quas ...
... A new research direction in low dimensional condensed matter physics that has attracted much recent attention is the study of two-dimensional (2D) topological quantum states of matter (e.g., fractional quantum Hall effects, chiral p-wave superfluids or superconductors, etc.) that support exotic quas ...
Von Neumann`s Impossibility Proof: Mathematics in - Philsci
... book’s first three chapters. But it should be noted already now that in his introductory remarks von Neumann does not declare that hidden variables are flatly impossible, but only that their introduction would conflict with what he considers basic general characteristics of quantum mechanics. In ch ...
... book’s first three chapters. But it should be noted already now that in his introductory remarks von Neumann does not declare that hidden variables are flatly impossible, but only that their introduction would conflict with what he considers basic general characteristics of quantum mechanics. In ch ...