Confined Carriers DRAGICA VASILESKA PROFESSOR ARIZONA STATE UNIVERSITY.

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Presentation transcript:

Confined Carriers DRAGICA VASILESKA PROFESSOR ARIZONA STATE UNIVERSITY

Outline Nanoelectronics Quantum Confined Structures: General Considerations Quantum Wells  Triangular: Si/SiO 2 Interface  Rectangular: Heterostructures

Nanotechnology/Nanoelectronics Nanotechnology is the design and construction of useful technological devices whose size is a few billionths of a meter Nanoscale devices will be built of small assemblies of atoms linked together by bonds to form macro-molecules and nanostructures Nanoelectronics encompasses nanoscale circuits and devices including (but not limited to) ultra-scaled FETs, quantum SETs, RTDs, spin devices, superlattice arrays, quantum coherent devices, molecular electronic devices, and carbon nanotubes.

Motivation for Nanoelectronics Negative resistance devices, switches (RTDs, molecular), spin transistors Single electron transistor (SET) devices and circuits Quantum cellular automata (QCA) Limits of Conventional CMOS technology Device physics scaling Interconnects Nanoelectronic alternatives? Issues Predicted performance improves with decreased dimensions, BUT Smaller dimensions-increased sensitivity to fluctuations Manufacturability and reproducibility Limited demonstration system demonstration New information processing paradigms Quantum computing, quantum info processing (QIP) Sensing and biological interface Self assembly and biomimetic behavior

Transport Regimes ‘Classical’ ‘Quantum’ Transport regime depends on length scale: l  -Phase coherence length l in -Inelastic mean free path l e -Elastic mean free path

P P Diffusive Transport L>>l  Phase Coherent Transport L<<l  Energy dissipation in active region Energy dissipation in contact

New Phenomena at the Nanoscale Quantum Confinement- small dimensions lead to quantum confinement and associated quantization of motion leading to discrete energy levels Quantum Interference- at dimensions smaller than the phase coherence length, the wave-like behavior of particles manifests itself, leading to reflection, refraction, tunneling, and other non- classical wave-like behavior Phase Coherent Transport- at dimensions smaller than the mean free path for scattering, transport is ballistic rather than diffusive Single Electron Effects- for small structures, the discrete nature of charge itself is important, and the associate energy for transfer of charge is non-negligible compared to the total energy of the system Spin Dependent Transport- Due to effects of quantum confinement, spin dependent phenomena may be enhanced.

Quantum Confined Structures: General Consideration Confinement in one dimension: Quantum Well, Quasi-two-dimensional electron gas (2DEG) Confinement in two dimensions: Quantum wire, quasi-one-dimensional system (1DEG) Confinement in all three directions: Quantum dot, artificial molecule. No degrees of freedom, completely discrete energy spectrum, singular density of states

Example 1 of Quantization: Quantization at the Si-SiO 2 Interface

Capacitance Degradation

Threshold Voltage Shift

Example 2 of Quantization: Quantum Wells and Heterostructures AAB CB VB QW c1 c2 hh1 hh2 lh1 Each state (c1, c2, hh1, hh2, etc. corresponds to the formation of a two- dimensional subband, which is free electron like in plane parallel to well.

Transfer Chamber Cryopump Surface Prep Chamber Ion Pump Growth Chamber LN2 Epitaxial Growth: MBE, MOCVD, MOMBE, MOVPE…

Epitaxial Layer Structure: Vertical Confinement TEM Cross Section

Band Diagrams of Heterostructures

Straddled – Type IStaggered – Type IIBroken – Type III There have been numerous attempts and models to predict band offsets. Band Allignments

k x, k y D E HH LH E Quasi-Two Dimensional System