CQT: Concepts of Quantum Transport
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| Abstract | Note: For an expanded version of these lectures see Datta's 2008 NCN@Purdue Summer School presentations on Nanoelectronics and the Meaning of Resistance.
In this series of four lectures (total length ~ 5-6 hours) Datta attempts to convey the physics of current flow in nanodevices in simple physical terms, stressing clearly what is understood and what is not. In Lecture 1, "Nanodevices and Maxwell's demon", Datta attempts to convey the subtle interplay of dynamics and thermodynamics that is the hallmark of transport physics using an electronic device reminiscent of the demon imagined by Maxwell in the nineteenth century to illustrate the limitations of the second law of thermodynamics. Lecture 2 ("Electrical Resistance: A simple model") explains many important concepts like the quantum of conductance using a simple model that Datta uses routinely to teach an undergraduate class on Nanoelectronics. Lecture 3 ("Probabilities, wavefunctions and Green's functions) describes the full quantum transport model touching on some of the most advanced concepts of non-equilibrium statistical mechanics including the Boltzmann equation and the non-equilibrium Green function (NEGF) formalism and yet keeping the discussion accessible to advanced undergraduates. Finally in Lecture 4 ("Coulomb blockade and Fock space") Datta explains the limitations of the current models and speculates on possible directions in which the field might evolve. Overall the objective is to convey an appreciation for state-of-the-art quantum transport models far from equilibrium, assuming no significant background in quantum mechanics or statistical mechanics. One-semester courses taught by the author on related material can be found at:
Text: S. Datta, Quantum Transport: Atom to Transistor, Cambridge (2005), ISBN 0-521-63145-9. Acknowledgements: Tehseen Raza.
No advanced background required. |
| Sponsored by | The Network for Computational Nanotechnology |
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| Lecture Number/Topic | Online Lecture | Video | Lecture Notes | Supplemental Material | Suggested Exercises |
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| CQT Introduction A short overview of this series of four lectures is given. |
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| CQT Lecture 1: Nanodevices and Maxwell's Demon Objective: To illustrate the subtle interplay of dynamics and thermodynamicsthat distinguishes transport physics. |
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| CQT Lecture 2: Electrical Resistance - A Simple Model Objective: To introduce a simple quantitative model for describing current flow in nanoscalestructures and relate it to well-known large scale properties like Ohm’s Law. |
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| CQT Lecture 3: Probabilities, Wavefunctions and Green Functions Objective: To extend the simple model from Lecture 2 into the full-blown model combines the NEGF (Non-Equilibrium Green Function) method with the Landauer approach. |
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| CQT Lecture 4: Coulomb blockade and Fock space Objective: To illustrate the limitations of the model described in Lectures 2, 3 and introduce a completely different approach based on the concept of Fock space. I believe this will be a key … |
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| McCoy Lecture: Nanodevices and Maxwell's Demon This is a video taped live lecture covering roughly the same material as lecture 1 of "Concepts of Quantum Transport". Video only. |
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| PASI Lecture: Nanodevices and Maxwell's Demon, Part 1 Pan American Advanced Study Institute (PASI) Lectures. This is part 1 of a video taped set of two one-hour live lectures covering roughly the same material as Lectures 1-3 of Concepts of … |
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| PASI Lecture: Nanodevices and Maxwell's Demon, Part 2 Pan American Advanced Study Institute (PASI) Lectures. This is part 2 of a video taped set of two one-hour live lectures covering roughly the same material as Lectures 1-3 of Concepts of … |
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| HCIS-15 Lecture: Nanodevices and Maxwell’s Demon The 15th International Conference on Nonequilibrium Carrier Dynamics in Semiconductors (HCIS-15) lecture. This 30 minute lecture covers roughly the same material as Lecture 1 of Concepts of … |
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How does the resistance of a conductor change as we shrink its length
all the way down to a few atoms? This is a question that has
intrigued scientists for a long time, but it is only during the last
twenty years that it has become possible for experimentalists to
provide clear answers, leading to enormous progress in our
understanding. There is also great applied interest in this question
at this time, since every computer we buy has about a billion
transistors that rely on controlling the flow of electrons through a
conductor a few hundred atoms in length.