• Study Resource
  • Explore Categories
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Fano resonances in the excitation spectra of semiconductor
Fano resonances in the excitation spectra of semiconductor

... favors narrow linewidths in the excitation spectrum by preventing the broadening from the alloy scattering. On the other hand, the double quantum-well structure allows a higher penetration of the heavy-hole wave function into the barrier resulting in a sizable oscillator strength for the hh3-cb1 tra ...
Spectral and spatial decomposition of lithospheric magnetic field models using spherical Slepian functions
Spectral and spatial decomposition of lithospheric magnetic field models using spherical Slepian functions

... One of the early attempts at bringing spatial selectivity to spherical-harmonic-based representations involved an approach reminiscent of ‘wavelet’ analysis (Simons et al. 1997). Spatially selective windows targeting a particular spectral degree range were designed, and a space-spectral analysis con ...
D:\Textbooks Reprint 2012-13\CD for States\12089
D:\Textbooks Reprint 2012-13\CD for States\12089

ppt - Harvard Condensed Matter Theory group
ppt - Harvard Condensed Matter Theory group

PHY2054_f11-solutions
PHY2054_f11-solutions

The Fourth Quantum Number
The Fourth Quantum Number

Large Local-Field Corrections in Optical Rotatory Power of Quartz and...
Large Local-Field Corrections in Optical Rotatory Power of Quartz and...

... which indicates that the local-field correction is negative and smaller than the macroscopic response. This conclusion is in reasonable agreement with the typical 210% correction for the dielectric constant. A similar result can be obtained for the second-harmonic coefficient. ...
End-of-Chapter Exercises
End-of-Chapter Exercises

charged geosynchronous debris perturbation
charged geosynchronous debris perturbation

Quantum Entanglement and Information Quantifier for Correlated
Quantum Entanglement and Information Quantifier for Correlated

E - umdberg
E - umdberg

Title A coaxial magnetic gear with halbach permanent
Title A coaxial magnetic gear with halbach permanent

Quantum Information and Quantum Computation
Quantum Information and Quantum Computation

... Over the last half century, the components of computers have gotten smaller by a factor of two every year and a half, the phenomenon known as Moore's law. In current computers, the smallest wires and transistors are coming close to a size of one hundred nanometers across, a thousand times the diamet ...
1 THE TECHNIQUE OF SIGNIFICABLES A proposed complete
1 THE TECHNIQUE OF SIGNIFICABLES A proposed complete

EEC 125 Electrical Eng`g Science 2 Theory - Unesco
EEC 125 Electrical Eng`g Science 2 Theory - Unesco

Lecture04: Gauss`s Law
Lecture04: Gauss`s Law

Chapter 19 Electric Charges, Forces, and Fields
Chapter 19 Electric Charges, Forces, and Fields

... a point halfway betweenthe charges q1 and q2. (b) Is the magnitude of the electric field halfway between q2 and q3 greater than, less than or the same as the electric field found in part (a)? (c) Find the magnitude of the electric field at the point specified in part (b). ...
On the correspondence principle
On the correspondence principle

... function become indistinguishable. Although their work is of great interest it does concentrate on the weak form of the correspondence principle. Finally, we observe that Greenbaum et al note in their work the conditions for weak QCT may need modification for systems with more than one dimension. Ou ...
Chapter 26
Chapter 26

Electric Fields i.e. The Electric Charge, Electric Force, and
Electric Fields i.e. The Electric Charge, Electric Force, and

Introduction to the Maxwell Garnett approximation: tutorial
Introduction to the Maxwell Garnett approximation: tutorial

Magnetic Fields
Magnetic Fields

QUANTUM SUPERPOSITION PRINCIPLE
QUANTUM SUPERPOSITION PRINCIPLE

Physics of Potassium Ion Channel Inactivation in Neurons
Physics of Potassium Ion Channel Inactivation in Neurons

Lecture16
Lecture16

< 1 ... 137 138 139 140 141 142 143 144 145 ... 661 >

Aharonov–Bohm effect

The Aharonov–Bohm effect, sometimes called the Ehrenberg–Siday–Aharonov–Bohm effect, is a quantum mechanical phenomenon in which an electrically charged particle is affected by an electromagnetic field (E, B), despite being confined to a region in which both the magnetic field B and electric field E are zero. The underlying mechanism is the coupling of the electromagnetic potential with the complex phase of a charged particle's wavefunction, and the Aharonov–Bohm effect is accordingly illustrated by interference experiments.The most commonly described case, sometimes called the Aharonov–Bohm solenoid effect, takes place when the wave function of a charged particle passing around a long solenoid experiences a phase shift as a result of the enclosed magnetic field, despite the magnetic field being negligible in the region through which the particle passes and the particle's wavefunction being negligible inside the solenoid. This phase shift has been observed experimentally. There are also magnetic Aharonov–Bohm effects on bound energies and scattering cross sections, but these cases have not been experimentally tested. An electric Aharonov–Bohm phenomenon was also predicted, in which a charged particle is affected by regions with different electrical potentials but zero electric field, but this has no experimental confirmation yet. A separate ""molecular"" Aharonov–Bohm effect was proposed for nuclear motion in multiply connected regions, but this has been argued to be a different kind of geometric phase as it is ""neither nonlocal nor topological"", depending only on local quantities along the nuclear path.Werner Ehrenberg and Raymond E. Siday first predicted the effect in 1949, and similar effects were later published by Yakir Aharonov and David Bohm in 1959. After publication of the 1959 paper, Bohm was informed of Ehrenberg and Siday's work, which was acknowledged and credited in Bohm and Aharonov's subsequent 1961 paper.Subsequently, the effect was confirmed experimentally by several authors; a general review can be found in Peshkin and Tonomura (1989).
  • studyres.com © 2026
  • DMCA
  • Privacy
  • Terms
  • Report