Tags: nanotransistors

Description

A nanotransistor is a transistor whose dimensions are measured in nanometers. Transistors are used for switching and amplifying electronic signals. When combined in the millions and billions, they can be used to create sophisticated programmable information processors.

Resources (141-160 of 417)

  1. ECE 656 Lecture 16: Solving the BTE: Magnetic Fields

    09 Nov 2009 | | Contributor(s):: Mark Lundstrom

    Outline:General solutionCurrent equationCoupled current equationsExampleSummary

  2. ECE 656 Lecture 22: Charged Impurity Scattering

    06 Nov 2009 | | Contributor(s):: Mark Lundstrom

    Online:ReviewScreeningBrooks-Herring approachConwell-Weisskopf approachDiscussionSummary / Questions

  3. ECE 656 Lecture 18: Strong Magnetic Fields

    05 Nov 2009 | | Contributor(s):: Mark Lundstrom

    OutlineMagnetoconductivity tensorResistivity tensorStrong B-fields: Landau levelsShubnikov-DeHaas Oscillations and QHESummary

  4. ECE 656 Lecture 19: Characteristic Times

    05 Nov 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Characteristic timesRelaxation Time Approximation and τr

  5. ECE 656 Lecture 20: Transmission and Backscattering

    05 Nov 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Transmission and mfpMFP and carrrier scatteringExtracting mean-free-paths from experiments

  6. ECE 656 Lecture 21: Scattering and Fermi's Golden Rule

    05 Nov 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Fermi’s Golden RuleExample: static potentialExample: oscillating potentialDiscussionSummary

  7. ECE 656 Exam 1 (Fall 2009)

    08 Oct 2009 | | Contributor(s):: Mark Lundstrom

  8. ECE 656 Lecture 14: Solving the BTE: 1D/RTA

    07 Oct 2009 | | Contributor(s):: Mark Lundstrom

    Outline:The RTA Solving the BTE: driftSolving the BTE: diffusionEnergy-dependent scattering timeRelation to LandauerDiscussionSummary

  9. ECE 656 Lecture 11: Discussion

    07 Oct 2009 | | Contributor(s):: Mark Lundstrom

    Outline:P-type conductors and thermoelectricsZT figure of meritMaximizing the “power factor”TE parameters for non-degenerate semiconductor

  10. ECE 656 Lecture 15: Solving the BTE - General Solution for B = 0

    06 Oct 2009 | | Contributor(s):: Mark Lundstrom

    General solution 2) Current equation 3) Coupled current equations 4) The RTA 5) Summary

  11. ECE 656 Lecture 17: BTE and Landauer

    02 Oct 2009 | | Contributor(s):: Mark Lundstrom

    Outline:BTE reviewTransport DistributionConnection to LandauerModesMean-free-pathSummary

  12. ECE 656 Lecture 10: The Drift-Diffusion Equation

    30 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Transport in the bulkThe DD equationIndicial notationDD equation with B-field

  13. ECE 656 Lecture 9: Coupled Current Equations

    28 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Onsager relationsMeasurement considerationsThermoelectric devices

  14. ECE 656 Lecture 8: Thermoelectric Effects

    27 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:IntroductionOne energy level formulationDistribution of energy levelsDiscussionSummary

  15. ECE 656 Lecture 7: 2 and 3D Resistors

    27 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Another view of the same problem2D resistorsDiscussion3D resistorsSummary

  16. ECE 656 Lecture 13: Solving the BTE: equilibrium and ballistic

    22 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Quick reviewEquilibrium BTEBallistic BTEDiscussionSummary

  17. Metal Oxide Nanowires as Gas Sensing Elements: from Basic Research to Real World Applications

    21 Sep 2009 | | Contributor(s):: andrei kolmakov

    Quasi 1-D metal oxide single crystal chemiresistors are close to occupy their specific niche in the real world of solid state sensorics. Potentially, the major advantage of this kind of sensors with respect to available granular thin film sensors will be their size and stable, reproducible and...

  18. ECE 656 Lecture 12: Boltzmann Transport Equation

    18 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:IntroductionSemi-classical electron dynamics Boltzmann Transport Equation (BTE) ScatteringDiscussionSummary

  19. ECE 656 Lecture 6: Discussion

    18 Sep 2009 | | Contributor(s):: Mark Lundstrom

    OutlineQuantum confinement and effective massBulk 1D transport and mfpPeriodic vs. Box boundary conditionsThermal velocities"Ballistic mobility"

  20. ECE 656 Lecture 5: 1D Resistors

    14 Sep 2009 | | Contributor(s):: Mark Lundstrom

    Outline:Review1D ballistic resistors1D diffusive resistorsDiscussionSummary