𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Thermoelectric and thermo-Coulomb effects in tunnel junctions

✍ Scribed by M. Amman; E. Ben-Jacob; J.L. Cohn


Publisher
Elsevier Science
Year
1992
Tongue
English
Weight
484 KB
Volume
171
Category
Article
ISSN
0375-9601

No coin nor oath required. For personal study only.


πŸ“œ SIMILAR VOLUMES


Observation of Coulomb Blockade Effects
✍ BrοΏ½ckl, H.; Rank, R.; Vinzelberg, H.; MοΏ½nch, I.; Kretz, L.; Reiss, G. πŸ“‚ Article πŸ“… 1997 πŸ› John Wiley and Sons 🌐 English βš– 280 KB

Narrow metal wires patterned on Si(100) wafers by conventional e-beam lithography have been subsequently mechanically modiÐed with an atomic force microscope. Using the line resistance as an indicator of the progress of the modiÐcation, narrow insulating gaps were successfully machined into the line

Coulomb oscillations in double metal tun
✍ L.J. Geerligs; M. Matters; J.E. Mooij πŸ“‚ Article πŸ“… 1994 πŸ› Elsevier Science 🌐 English βš– 152 KB

The Coulomb blockade of electron tunneling through two tunnel junctions in series can be suppressed periodically by applying a gate voltage to the central island. The resulting conductance peaks ("Coulomb oscillations") have been studied in aluminum-oxide-aluminum tunnel junctions. For decreasing te

Coulomb blockade and higher order tunnel
✍ Reiko Kitawaki; Fujio Wakaya; Shuichi Iwabuchi πŸ“‚ Article πŸ“… 1999 πŸ› Elsevier Science 🌐 English βš– 291 KB

A microscopic theory for ultrasmall ferromagnetic double tunnel junctions is proposed, which selfconsistently describes the higher order tunneling processes as well as the charged states of the islands for arbitrary environmental impedance. Such a theory is indispensable to understanding of the phys

Observability of the coulomb blockade in
✍ M.H. Devoret; D. Esteve; H. Grabert; G.-L. Ingold; H. Pothier; C. Urbina πŸ“‚ Article πŸ“… 1990 πŸ› Elsevier Science 🌐 English βš– 320 KB

The finite temperature I-V-;:haracteristic of a normal tunnel junction coupled to its electromagnetic environment is calculated. It is shown that due to quantum fluctuations of the charge the Coulomb gap is only observable provided the impedance Z(w) of the environment exceeds the resistance quantum