• 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
CHAPTER 6 Magnetic fields
CHAPTER 6 Magnetic fields

Line junctions in the quantum Hall effect - Penn Physics
Line junctions in the quantum Hall effect - Penn Physics

r - UNL CMS
r - UNL CMS

A simple experiment for discussion of quantum interference and
A simple experiment for discussion of quantum interference and

WAVE PARTICLE DUALITY, THE OBSERVER AND
WAVE PARTICLE DUALITY, THE OBSERVER AND

... A well-known thought experiment, which played a vital role in the history of quantum mechanics (for example, see the discussion on Einstein's version of this experiment), demonstrated that if particle detectors are positioned at the slits, showing through which slit a photon goes, the interference p ...
Electric Field Control of Magnetoresistance in InP Nanowires with
Electric Field Control of Magnetoresistance in InP Nanowires with

- RZ User
- RZ User

Electromagnetic waves in vacuum.
Electromagnetic waves in vacuum.

Electrostatics of Nanowires and Nanotubes: Application for Field
Electrostatics of Nanowires and Nanotubes: Application for Field

Wednesday, Sept. 28, 2005
Wednesday, Sept. 28, 2005

and q - LSU Physics
and q - LSU Physics

... Electric field lines always start at and are directed away from positive charges and always end at and are directed toward negative charges. But what would the electric field look like in a region of ...
test charge
test charge

unit 21: electrical and gravitational potential
unit 21: electrical and gravitational potential

Syllabus Science Physics Sem-3-4 (wef.2012-13)
Syllabus Science Physics Sem-3-4 (wef.2012-13)

The demagnetizing field of a non
The demagnetizing field of a non

The Quantum Mechanics of Angular Momentum
The Quantum Mechanics of Angular Momentum

課堂討論問題
課堂討論問題

... be 1.60 × 1019 C. What can we conclude from the fact that no smaller charges have been measured? a) Charge is quantized. b) Electrons are conserved. c) Charge is conserved. d) Electrons have the smallest unit of charge. e) Charge is the same as mass. ...
Multiscale theory of finite-size Bose systems: Implications for collective
Multiscale theory of finite-size Bose systems: Implications for collective

... BECs with long-range dipolar interactions have also generated much interest 关26,27兴. In the present study, we attempt to rigorously determine the limiting behavior of the wave function for boson QCs as ␧ → 0. The objective is to develop a theory of boson droplets by integrating these notions into a ...
Chapter 4 SINGLE PARTICLE MOTIONS
Chapter 4 SINGLE PARTICLE MOTIONS

Applications of Gauss Law
Applications of Gauss Law

... Charge configurations with planar symmetry include uniform 2D sheets, uniform slabs of finite thickness, as well as “sandwiches” of such sheets and slabs. In Cartesian coordinates (x, y, z), a general configuration with planar symmetry has 3D charge density ρ(x, y, z) which depends only on z but not ...
Analysis of Simple Charged Particle Systems that Exhibit Chaos
Analysis of Simple Charged Particle Systems that Exhibit Chaos

... result is that changing electric fields induce magnetic fields, and vice versa. Furthermore, the magnetic and electric fields can have a number of configurations depending on the physical situation that generates them. For the problems in this thesis, the effects of the full Maxwell’s equations are ...
Spin-based quantum computing using electrons on liquid helium
Spin-based quantum computing using electrons on liquid helium

Electromagnetic Waves
Electromagnetic Waves

electromagnetic waves in periodic structures
electromagnetic waves in periodic structures

... the axial propagation constant does not lie in or close to certain "forbidden regions," which will be discussed later. ...
L. Bell*, et. al., "THz emission by Quantum Beating in a Modulation
L. Bell*, et. al., "THz emission by Quantum Beating in a Modulation

< 1 ... 168 169 170 171 172 173 174 175 176 ... 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