Energy-related Problems - Research Laboratory of Electronics
... a conventional thermoelectric and the very thin junction region acts as a material with an anomalously high thermopower. The thin (micron) junction region in this case dominates the thermally induced voltage of the thick (millimeter) solid gap region. This is an important result, as it points to the ...
... a conventional thermoelectric and the very thin junction region acts as a material with an anomalously high thermopower. The thin (micron) junction region in this case dominates the thermally induced voltage of the thick (millimeter) solid gap region. This is an important result, as it points to the ...
Photoassociation of ultracold LiRb molecules: Observation of high efficiency
... LiRb∗ molecules which either spontaneously decay to LiRb molecules in the electronic ground state or to free Li and Rb atoms with high kinetic energies. Both mechanisms result in loss of the Li and Rb atoms from the MOT leading to a decrease in the MOT fluorescence. The formation of LiRb∗ molecules ...
... LiRb∗ molecules which either spontaneously decay to LiRb molecules in the electronic ground state or to free Li and Rb atoms with high kinetic energies. Both mechanisms result in loss of the Li and Rb atoms from the MOT leading to a decrease in the MOT fluorescence. The formation of LiRb∗ molecules ...
Quantum dynamics study of fulvene double bond photoisomerization: The
... drogen atoms in Figure 1). The two isomers are connected by a double bond isomerization. They are labeled FC, which stands for Franck-Condon geometry, and FC . Every point on the seam plotted in Figure 1 is a conical intersection if another coordinate (the interstate coupling coordinate, see below) ...
... drogen atoms in Figure 1). The two isomers are connected by a double bond isomerization. They are labeled FC, which stands for Franck-Condon geometry, and FC . Every point on the seam plotted in Figure 1 is a conical intersection if another coordinate (the interstate coupling coordinate, see below) ...
Author`s personal copy
... signal I sig of which the upper limit is described by ( P /hν )e (e is unit charge, P the incident light power and hν the photon energy). This gives photoconductive detectors the upper limit of D ∗ . On the other hand, in the QD detector, the single photon absorption is converted to a long-lived uni ...
... signal I sig of which the upper limit is described by ( P /hν )e (e is unit charge, P the incident light power and hν the photon energy). This gives photoconductive detectors the upper limit of D ∗ . On the other hand, in the QD detector, the single photon absorption is converted to a long-lived uni ...
Experimental - AIP FTP Server
... polarisation vector, phot, at any user selected angle, , relative to the TOF axis. ...
... polarisation vector, phot, at any user selected angle, , relative to the TOF axis. ...
Cotunneling in the ν Robert Zielke, Bernd Braunecker,
... state in which the elementary excitations obey non-Abelian fractional statistics.1–7 Numerical simulations testing these proposals have remained inconclusive,8–13 mainly due to finite size limitations. A proof of the nature of the 5/2-FQHS should therefore come from experiments.14 As a first indicat ...
... state in which the elementary excitations obey non-Abelian fractional statistics.1–7 Numerical simulations testing these proposals have remained inconclusive,8–13 mainly due to finite size limitations. A proof of the nature of the 5/2-FQHS should therefore come from experiments.14 As a first indicat ...
Two-Dimensional Schrodinger Scattering and Electron Transport in Graphene
... nature of the primary structure of Graphene as replicated throughout the lattice. In this sense, each primary element of Graphene is analogous to the structure of Benzene from which the concept of de-localised electrons was first derived. The de-localised electrons represent a repulsive electrostati ...
... nature of the primary structure of Graphene as replicated throughout the lattice. In this sense, each primary element of Graphene is analogous to the structure of Benzene from which the concept of de-localised electrons was first derived. The de-localised electrons represent a repulsive electrostati ...
Electrically tunable hole g factor of an optically active quantum dot
... We demonstrate here that the hole g factor in a quantum dot is very sensitive to an electric field F (along the growth direction z) when the magnetic field B is applied in-plane, the magnetic field direction required to generate a coherent hole spin. On the one hand, the sensitivity to electric fiel ...
... We demonstrate here that the hole g factor in a quantum dot is very sensitive to an electric field F (along the growth direction z) when the magnetic field B is applied in-plane, the magnetic field direction required to generate a coherent hole spin. On the one hand, the sensitivity to electric fiel ...
Undergraduate Quantum Chemistry Written by Jussi Eloranta
... they must be particles. In the case of photons such experiment can be made using the single photon counting technique. The concept of particle is familiar to us from classical physics. A classical particle has a well defined position and momentum. Let’s consider behavior of photons as an example. Ph ...
... they must be particles. In the case of photons such experiment can be made using the single photon counting technique. The concept of particle is familiar to us from classical physics. A classical particle has a well defined position and momentum. Let’s consider behavior of photons as an example. Ph ...
Chapter 2 Atoms, Molecules, and Ions
... Cations are positive and are formed by elements on the left side of the periodic chart. Anions are negative and are formed by elements on the right Atoms, Molecules, side of the periodic chart. and Ions ...
... Cations are positive and are formed by elements on the left side of the periodic chart. Anions are negative and are formed by elements on the right Atoms, Molecules, side of the periodic chart. and Ions ...
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.