Difference between revisions of "Nanoelectronics"
From apm
(basic page) |
(→External links: reorder + added link to WP page about Superexchange) |
||
| (7 intermediate revisions by the same user not shown) | |||
| Line 49: | Line 49: | ||
* [https://en.wikipedia.org/wiki/Category:Two-dimensional_nanomaterials Category:Two-dimensional_nanomaterials] | * [https://en.wikipedia.org/wiki/Category:Two-dimensional_nanomaterials Category:Two-dimensional_nanomaterials] | ||
---- | ---- | ||
| − | * [https://en.wikipedia.org/wiki/Dirac_fermion Dirac_fermion] | + | * '''[https://en.wikipedia.org/wiki/Dirac_fermion Dirac_fermion] – Effect of low dimensional constraint.''' |
| + | * '''[https://en.wikipedia.org/wiki/Luttinger_liquid Luttinger_liquid] – Electrons in a 1D conductor.''' | ||
| + | * [https://en.wikipedia.org/wiki/Fermi_liquid_theory Fermi liquid theory] | ||
| + | * '''[https://en.wikipedia.org/wiki/Mermin%E2%80%93Wagner_theorem Mermin–Wagner theorem] – Effect of low dimensional constraints.''' | ||
| + | * '''[https://en.wikipedia.org/wiki/Avoided_crossing Avoided crossing]''' | ||
---- | ---- | ||
* [https://en.wikipedia.org/wiki/Graphene Graphene] & [[https://en.wikipedia.org/wiki/Graphene_nanoribbon Graphene nanoribbon]] | * [https://en.wikipedia.org/wiki/Graphene Graphene] & [[https://en.wikipedia.org/wiki/Graphene_nanoribbon Graphene nanoribbon]] | ||
| Line 61: | Line 65: | ||
* [https://en.wikipedia.org/wiki/2D_silica 2D silica] | * [https://en.wikipedia.org/wiki/2D_silica 2D silica] | ||
* [https://en.wikipedia.org/wiki/Transition_metal_dichalcogenide_monolayers Transition metal dichalcogenide monolayers] | * [https://en.wikipedia.org/wiki/Transition_metal_dichalcogenide_monolayers Transition metal dichalcogenide monolayers] | ||
| + | |||
| + | === Misc === | ||
| + | |||
| + | * '''[https://en.wikipedia.org/wiki/Carrier_scattering#Phonon_scattering Carrier_scattering#Phonon_scattering]''' | ||
| + | * [https://en.wikipedia.org/wiki/Electron_mobility Electron mobility] | ||
| + | * '''[https://en.wikipedia.org/wiki/Electron_scattering Electron scattering]''' | ||
| + | ---- | ||
| + | '''Magnetic:''' | ||
| + | * [https://en.wikipedia.org/wiki/Bohr_magneton Bohr magneton] | ||
| + | * [https://en.wikipedia.org/wiki/Spin_pumping Spin pumping] | ||
| + | * [https://en.wikipedia.org/wiki/Spin-transfer_torque Spin-transfer torque] | ||
| + | * [https://en.wikipedia.org/wiki/Superexchange Superexchange] | ||
Latest revision as of 16:50, 13 August 2023
Nanoelectronics is much more difficult tho analyze than nanomechanics as it behaves much more quanummechanically and allows less simpplifying engineering style separation of concerns thus less back on the envelope conservative estimations.
See: Nanomechanics is barely mechanical quantummechanics & Non mechanical technology path.
Still nanoelectronics will be extremely useful and thus can't really be ignored.
This page is just meant as a starting point to learn about the subject in the context of APM and gem-gum-tec.
Nanowires and ribbons being of obvious interest also bring special interest to theories describing the cases of 1D and 2D electon gas.
A lot of exotic phenomena can be likely created via:
- constraint of the electron gas to 1D/2D
- atomic precision removing crystal defects as scatter-sources (phonons still can scatter electrons)
- atomically precise patterning and chemical additions (repetitive surface structures)
- well metastable highly strained bonds
- applied pressure positive or negative pressure (comression or tension) See: High pressure
The exotic phenomena that are likely creatable include but are not limited to:
- Very fast electron motion due to low effective electron masses (cone in dispersion relation)
- Superconduction at high temperatures (perhaps even at or beyond room temperature)
- Especially stable spin states
- ...
Contents
Related
- Difference in difficulty to nanomechanics:
Nanomechanics is barely mechanical quantummechanics - Non mechanical technology path
- Superconductors
- Electronic transitions
- Fun with spins
External links
Nanoelectronics theories
- Mott insulator
"A Mott transition is a transition from a metal to an insulator, driven by the strong interactions between electrons. One of the simplest models that can capture Mott transition is the Hubbard model." & "Mott insulators … have applications in thin-film magnetic heterostructures and the strong correlated phenomena in high-temperature superconductivity" - Mott criterion
- Charge-transfer insulators
Nanoelectronic materials
- Dirac_fermion – Effect of low dimensional constraint.
- Luttinger_liquid – Electrons in a 1D conductor.
- Fermi liquid theory
- Mermin–Wagner theorem – Effect of low dimensional constraints.
- Avoided crossing
- Graphene & [Graphene nanoribbon]
- Silicene (tuneable bandgap)
- Germanene (no bandgap)
- Stanene (topological insulator and perhaps roomtemp superconduction on edges??)
- Plumbene
Misc
Magnetic:
