|Statement||edited by D.C. Glattli, M. Sanquer, J. Trân Thanh Vân.|
|Series||Moriond condensed matter physics|
|Contributions||Glattli, D. C., Sanquer, M., Tran, J. Thanh Van., Rencontre de Moriond (29th : 1994 : Villars-sur-Ollon, Switzerland)|
|LC Classifications||QC176.8.E4 M62 1994|
|The Physical Object|
|Pagination||xii, 441 p. :|
|Number of Pages||441|
|LC Control Number||98147454|
Proceedings of the XXIXth RENCONTRE DE MORlaND Series: Moriond Condensed Matter Physics Villars sur Ollon, Switzerland January , COULOMB AND INTERFERENCE EFFECTS IN SMALL ELECTRONIC STRUCTURES edited by. Electronic Systems, in D. C. Glattli et al. (editors), Coulomb and Interference Effects in Small Electronic Structures, Editions Frontiers, France-press, pp. (). 6. Y. Gefen and A. Kamenev, On the Role of the Statistical Ensemble in the Dynamics and Thermodynamics of Finite Disordered Systems in H. A. Cerdeira et al. (editors). Distinct Signatures For Coulomb Blockade and Aharonov-Bohm Interference in Electronic Fabry-Perot Interferometers Article (PDF Available) in Physical review. B, Condensed matter 79(24) December. Coulomb’s law calculates the magnitude of the force F between two point charges, q1 and q2, separated by a distance r. In SI units, the constant k is equal to. k = ×N⋅m2 C2 ≈ ×N⋅m2 C2. k = × 10 9 N ⋅ m 2 C 2 ≈ × 10 9 N ⋅ m 2 C 2. The electrostatic force is a vector quantity and is expressed in units.
A telling example is the interplay of Kondo physics and quantum interference in "side-coupled" or "hanging-dot" configurations,    leading to a variety of. Interference effects in the Coulomb blockade regime: Current blocking and spin preparation in symmetric nanojunctions Article (PDF Available) in Physical review. B, Condensed matter 82(12) July. We investigate the ionization dynamics of atoms irradiated by an intense laser field using a semiclassical model that includes magnetic Lorentz force in the rescattering process. We find that, the electrons tunneled with different initial transverse momenta (i.e., perpendicular to the instantaneous electric field direction) distributed on a specific circle in the momentum plane . The coulomb explosion model is the first to have been proposed to explain the phase changes, and it was initially assumed that the model is applicable to insulators [56,57].According to this model, a positively charged region of a few nanometers is created by ionization of target atoms, after the passage of SHI (Fig. ).The coulomb repulsion between these ions in the small .
Transport in Nanostructures. DAVID K. FERRY and STEPHEN M. GOODNICK. Cambridge University Press, New York, xii, pp., illus. $ ISBN Cambridge Studies in Semiconductor Physics and Microelectronic Engineering, 6. This year jubilee for the transistor has given us many reviews on the development of this remarkable solid-state device. K. Miyaji, T. Hiramoto, in Comprehensive Semiconductor Science and Technology, Coulomb blockade effect. The Coulomb blockade effect is the most fundamental phenomenon used not only in SETs/SHTs but also in single-electron memories, single-electron transport devices, and so on, to control the motion of a single electron. In this section, an . Besides Coulomb blockade, the electron-electron interaction cause momentum-exchange which leads to the well known Coulomb drag effect in double-layer structures  . Coulomb (deﬁned by the deﬁnition of current i.e. a Coulomb per second), length measured in meters, and force in Newtons, then κ is set equal to 1 4πǫ0. In this expression, ǫ0 is the permittivity of free space, and has the value × 10−12 farad/m. These units are theFile Size: KB.