Title Goes Here
... the lowest bound state. At higher ne, we observed the metal-insulator crossover where the trion peak evolves to the typical single absorption onset of the band-toband transition. In this crossover region, we found a double absorption peak structure corresponding to Fermi edge at low temperature and ...
... the lowest bound state. At higher ne, we observed the metal-insulator crossover where the trion peak evolves to the typical single absorption onset of the band-toband transition. In this crossover region, we found a double absorption peak structure corresponding to Fermi edge at low temperature and ...
drastically
... the optical dipole moment of the a QD is 1 to 2 orders of magnitude larger [15, 28]. Although a QD is embedded in a complex solid state environment, the problems which occur in higher dimensional semiconductor structures, such as many body effects [12], are strongly suppressed due to the three dimen ...
... the optical dipole moment of the a QD is 1 to 2 orders of magnitude larger [15, 28]. Although a QD is embedded in a complex solid state environment, the problems which occur in higher dimensional semiconductor structures, such as many body effects [12], are strongly suppressed due to the three dimen ...
Relativistic Effects in Atomic Spectra
... The history of physics has shown an interesting progress of the comprehension of manyparticle systems: in classical mechanics, the three-body problem has been known not being solvable generally. In electrodynamics, also the two-body case has become unsolvable. When quantum mechanics was emerging, ne ...
... The history of physics has shown an interesting progress of the comprehension of manyparticle systems: in classical mechanics, the three-body problem has been known not being solvable generally. In electrodynamics, also the two-body case has become unsolvable. When quantum mechanics was emerging, ne ...
Electronic structure of molecular van der Waals complexes with
... to describe the tunneling through various flat-lying alkyl derivatives on HOPG under typically used experimental conditions.4–16 Electrons from a metallic STM-tip tunnel through a molecule into the conducting substrate, or vice versa. A schematic energy diagram is displayed in Fig. 1. The workfuncti ...
... to describe the tunneling through various flat-lying alkyl derivatives on HOPG under typically used experimental conditions.4–16 Electrons from a metallic STM-tip tunnel through a molecule into the conducting substrate, or vice versa. A schematic energy diagram is displayed in Fig. 1. The workfuncti ...
2 Phase Diagram of 2DES on Liquid Helium
... through the excitation of normal modes in the radio frequency range 10 MHz-1GHz. The normal mode spectra are expected to undergo a radical change at the transition from liquid to crystal, the so-called Wigner transition. This difference is due to coupling between 2DES modes and those of liquid heliu ...
... through the excitation of normal modes in the radio frequency range 10 MHz-1GHz. The normal mode spectra are expected to undergo a radical change at the transition from liquid to crystal, the so-called Wigner transition. This difference is due to coupling between 2DES modes and those of liquid heliu ...
Decoherence in Solid State Qubits
... A good example of a qubit is the spin 1/2. In order to explain the necessity to use complex number α and β to characterize the state of the qubit, we describe an interference procedure for a spin 1/2 particle. Suppose we prepare the spin in the state |ψ0 i = | ↑i, that is with probability 1 to find ...
... A good example of a qubit is the spin 1/2. In order to explain the necessity to use complex number α and β to characterize the state of the qubit, we describe an interference procedure for a spin 1/2 particle. Suppose we prepare the spin in the state |ψ0 i = | ↑i, that is with probability 1 to find ...
Quantum many-particle electron transport in time-dependent systems with Bohmian trajectories by Alfonso Alarc´
... Schematic representation of the I-V curve of a typical RTD. The resonant energy inside the quantum well acts like an energetic filter that lets the electrons from the source to arrive at the drain. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . RTD Current-voltage characte ...
... Schematic representation of the I-V curve of a typical RTD. The resonant energy inside the quantum well acts like an energetic filter that lets the electrons from the source to arrive at the drain. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . RTD Current-voltage characte ...
FERMI-HUBBARD PHYSICS WITH ATOMS IN AN OPTICAL LATTICE1
... assumes a single static band and local interactions between the particles (13; 14; 15). Yet, the question as to whether the ground state of the two-dimensional Fermi-Hubbard model supports d-wave superfluidity or superconductivity (16) has so far defied theoretical explanation - despite 20 years of ...
... assumes a single static band and local interactions between the particles (13; 14; 15). Yet, the question as to whether the ground state of the two-dimensional Fermi-Hubbard model supports d-wave superfluidity or superconductivity (16) has so far defied theoretical explanation - despite 20 years of ...
Chemical Equations
... Note, there appear to be more oxygen atoms, fewer hydrogen atoms at the end that at the beginning! ...
... Note, there appear to be more oxygen atoms, fewer hydrogen atoms at the end that at the beginning! ...
Ionization
Ionization is the process by which an atom or a molecule acquires a negative or positive charge by gaining or losing electrons to form ions, often in conjunction with other chemical changes. Ionization can result from the loss of an electron after collisions with sub atomic particles, collisions with other atoms, molecules and ions, or through the interaction with light. Heterolytic bond cleavage and heterolytic substitution reactions can result in the formation of ion pairs. Ionization can occur through radioactive decay by the internal conversion process, in which an excited nucleus transfers its energy to one of the inner-shell electrons causing it to be ejected.