By Supriyo Datta
Everyone seems to be accustomed to the fantastic functionality of a contemporary shrewdpermanent mobilephone, powered by means of a billion-plus nanotransistors, every one having an energetic zone that's slightly a couple of hundred atoms in size. those lecture notes are a few less-appreciated derivative of the microelectronics revolution, specifically the deeper realizing of present movement, and gadget operation that it has enabled, which types the foundation for a brand new method of shipping difficulties. The ebook assumes little or no historical past past linear algebra and differential equations, and is meant to be available to an individual in any department of technology or engineering.
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Additional resources for Lessons from Nanoelectronics: A New Perspective on Transport
Is Conductivity proportional to Electron Density? 5. Quantized Conductance 6. 1. 2. Currents in Terms of Non-Equilibrium Potentials 7. What about Drift? 1. 2. 3. 4. The Two Potentials 8. 1. 2. 3. 4. 5. Extended Channel Model 9. 1. 2. Old Topics in New Light 10. 1. 2. 3. 4. “Delta Function” Thermoelectric 11. 1. 2. Thermal Conductivity 12. 1. 2. Büttiker Formula 13. 1. 2. 3. 4. Non –Reciprocal Circuits 14. 1. 2. 3. 4. Polarizers and Analyzers 15. 1. 2. Onsager Relations 16. 1. 2. 3. 4. 5. Alternative Expression for Entropy 17.
Ballistic and Diffusive Transport 5. Conductivity 6. Diffusion Equation for Ballistic Transport 7. What about Drift? 8. Electrostatics is Important 9. Smart Contacts II. Old Topics in New Light 10. Thermoelectricity 11. Phonon Transport 12. Measuring Electrochemical Potentials 13. Hall Effect 14. Spin Valve 15. Kubo Formula 16. Second Law 17. Fuel Value of Information III. Contact-ing Schrödinger 18. The Model 19. Non-Equilibrium Green’s Functions (NEGF) 20. Can Two Offer Less Resistance than One?
3. This is what makes the bottom-up approach so powerful in clarifying transport problems in general. But before we talk further about the conductance of an elastic resistor, let us address an important conceptual issue. Since current flow (I) through a resistor (R) dissipates a Joule heat of I2R per second, it seems like a contradiction to talk of an elastic resistor where electrons do not lose energy? The point to note is that while the electron does not lose any energy in the channel of an elastic resistor, it does lose energy both in the source and the drain and that is where the Joule heat gets dissipated.
Lessons from Nanoelectronics: A New Perspective on Transport by Supriyo Datta