Memristors by Quantum Mechanics - nanoqed：忆阻器的量子力学nanoqed.ppt

Questions Papers Email: nanoqed@ 20 IEEE 12th Inter. Conf. on Nanotechnology: Inter. Conv. Ctr., Birmingham UK, Aug.20-23, 2012 * Enter speaker notes here. * * * * * Enter speaker notes here. Heat Transfer in Nanoelectronics by Quantum Mechanics Thomas Prevenslik QED Radiations Discovery Bay, Hong Kong IEEE 12th Inter. Conf. on Nanotechnology: Inter. Conv. Ctr., Birmingham UK, Aug.20-23, 2012 1 Today, Fourier’s equation based on classical physics is routinely applied to heat transfer in nanoelectronics - resistors, capacitors, and inductors - having submicron dimensions. However, unphysical results are found. Memristors require a undefined source of space charge ( Williams – Stanford ) Resistance change in PCRAM devices caused by melting ( Goodson – Stanford ) 1/f noise is created by free electron collisions ( Hooge Relation – Philips Research ) [1] L. O. Chua, “Memristor - the missing circuit element,” IEEE Trans. Circuit Theory, vol. 18, pp. 507–519, 1971. Introduction 2 IEEE 12th Inter. Conf. on Nanotechnology: Inter. Conv. Ctr., Birmingham UK, Aug.20-23, 2012 Proposal Heat transfer in nanoelectronics is a QM effect that conserves Joule heat by creating QED photons instead of increasing temperature that produce charge by the photoelectric effect. QM = Quantum Mechanics QED = Quantum electrodynamics In this talk, I argue QM creates charge in nanoelectronics instead of the classical increase in temperature IEEE 12th Inter. Conf. on Nanotechnology: Inter. Conv. Ctr., Birmingham UK, Aug.20-23, 2012 3 IEEE 12th Inter. Conf. on Nanotechnology: Inter. Conv. Ctr., Birmingham UK, Aug.20-23, 2012 Theory Heat Capacity of the Atom Conservation of Energy TIR Confinement QED Induced Heat Transfer 4 Heat Capacity of the Atom 5 Nanostructures kT 0.0258 eV Classical Physics (kT 0) QM (kT = 0) IEEE 12th Inter. Conf. on