NANO-technologies and the Physics of the Missing Scale Stanislav ordin 2025

[Audio] NANO-technologies and the Physics of the Missing Scale Stanislav ordin 2025.

[Audio] Main Characteristics of THERMOELECTRIC - Key points in UNDERSTANDING NANO 1821–Seebeck, 1834-Peltier, 1931- Onzager, 1934-Ioffe, 1947-Prigozhin, 2017-Ordin.

[Audio] Einstein's view of the world. Some equations of Classical Physics can be rewritten in operator form. Albert Einstein., Planetary system Atom Physics has stepped over NANO.

[Audio] 1.0. Elements imbalance energy. 1.1. Principle Curie's symmetry and Cassimere - Onzager. 1.2. locality-measurability-detectability. 1.3. Temperature and thermoelectric waves. 1.4. Thermoelectric model Ioffe-Stilbans for dirty semeconductors. 1.5. Indirect transformation of energy. 1.6 Thermoelectric Anomalies 1.7. size thermoelectric effect. 1.8. Photo- thermo-electric effect. --------------------------------------------------------------------------------- 2.1. macroscopics in to microscopics. 2.2. Local currents -spatial transition. 2.3. Some additional results probes local termo-Emf. Brief list of missed issues.

[Audio] 1.1. The principle of symmetry of Curie and Kazimir - Onzager..

[Audio] Phenomenology is an ELEMENTARY description of a Phenomenon. Descriptions of three Phenomenons have elements that are invariant for all and must be taken into account at the micro level..

[Audio] 1.8. Photo thermoelectric effect. Injection of the main carriers of hot area p-n junction.

[Audio] 2.1. macroscopics in to microscopics. The measurability of quantum effects has not caused such "surprise ban" what has arisen in the first attempts of interpretation of local thermoelectric effects. Therefore it was also necessary to recheck a lot of things in to macroscopic before starting the analysis of actually local thermoelectric effects. But if L.S. Stilbans referred in the beginning to the fact that it not thermoelectricity, and thermoemission, after discussion with A.I. Anselm whose work "Vacuum thermoelement" became basis of thermoemission of other arguments against, except "You correct the model Ioffe!", at M.V. Vedernikov did not remain..

[Audio] Feynman Cellular Automaton Implemented by NANO-Technologies.

[Audio] von Neumann-Conway cellular automaton - The Game of LIFE.

[Audio] Schematic representation of resonance frequencies..

[Audio] A jump in the electrical conductivity of dehydrated mordenite when liquid metal is introduced into its 6 A channels against the background of an increase in the electrical conductivity of the metal coating..

[Audio] Lattice of concentration solitons with a moiré pattern of the crystal lattice between them and giant spatial dispersion in incommensurate quasicrystals of higher manganese silicide in the region of plasmon-phonon resonance..

[Audio] One-dimensionally incommensurate sublattices of higher manganese silicide.

[Audio] Lattice oscillators of highly ordered samples of rhombohedral (a, c) and cubic (b) boron nitride and weakly ordered samples of hexagonal boron nitride (d)..

[Audio] 1.7. size thermoelectric effect. Diffusion termo-EMF it is equal to small diffusion difference between average energy of Fermi and energy in stream μ , barrier termo-EMF order of height of potential barrier EG..

[Audio] 1.7. size thermoelectric effect. Barrier termo-EMF prevails at scales about and less than length of free run of electrons, but currents are not described by Richardson's formula..

[Audio] 1.7. size thermoelectric effect. (Statics) At the set direction of heat flux the polarity diffusion termo-EMF is set by the sign of the main carriers of current, barrier termo-EMF - is familiar the main carriers of hot facing injected through p-n junction..

[Audio] Thanks for attention. Thanks for attention.