<--- Back to Details
First PageDocument Content
Electronic band structure / Electron / Ludwig Boltzmann / Mercury telluride / Insulator / Introduction to quantum mechanics / Zeeman effect / Band gap / Quantum mechanics / Physics / Topological insulator / Spintronics
Date: 2015-04-30 23:12:38
Electronic band structure
Electron
Ludwig Boltzmann
Mercury telluride
Insulator
Introduction to quantum mechanics
Zeeman effect
Band gap
Quantum mechanics
Physics
Topological insulator
Spintronics

Berry Curvature as a Multi-Band Effect in Boltzmann Equations Asger Johannes Skjøde Bolet Supervisor: Jens Paaske

Add to Reading List

Source URL: qdev.nbi.ku.dk

Download Document from Source Website

File Size: 697,74 KB

Share Document on Facebook

Similar Documents

Distribution A Approved for Public Release; Distribution is Unlimited Photon Counting LADAR  M. J. Halmos, R. A. Reeder, B. Boland

Distribution A Approved for Public Release; Distribution is Unlimited Photon Counting LADAR M. J. Halmos, R. A. Reeder, B. Boland

DocID: 1qRJB - View Document

Joint CQSE and CASTS Seminar Weekly Seminar Nov. 27, 2015 (Friday) TIME Nov. 27, 2015, 14:30 ~ 15:30 TITLE

Joint CQSE and CASTS Seminar Weekly Seminar Nov. 27, 2015 (Friday) TIME Nov. 27, 2015, 14:30 ~ 15:30 TITLE

DocID: 1neo4 - View Document

PDF Document

DocID: 1gwRu - View Document

2 – 11 µm IR PHOTOELECTROMAGNETIC DETECTORS OPTICALLY IMMERSED PEMI Series  Example of D* vs Wavelength λ for PEMI Series HgCdTe Detectors. Spectral Characteristics

2 – 11 µm IR PHOTOELECTROMAGNETIC DETECTORS OPTICALLY IMMERSED PEMI Series Example of D* vs Wavelength λ for PEMI Series HgCdTe Detectors. Spectral Characteristics

DocID: 1fLQt - View Document

Appl. Phys. B 92, 343–Applied Physics B DOI: s00340y

Appl. Phys. B 92, 343–Applied Physics B DOI: s00340y

DocID: 1fuA3 - View Document