• 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
Lecture16
Lecture16

Zahn, M. and H.A. Haus, Contributions of Prof. James R. Melcher to Engineering Education, Journal of Electrostatics 34, pp. 109-162, March 1995
Zahn, M. and H.A. Haus, Contributions of Prof. James R. Melcher to Engineering Education, Journal of Electrostatics 34, pp. 109-162, March 1995

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

Chapter 12: Electrostatic Phenomena 1. An electron situated near
Chapter 12: Electrostatic Phenomena 1. An electron situated near

Electric and magnetic fields of a toroidal dipole in
Electric and magnetic fields of a toroidal dipole in

NO CELL PHONES, TEXT MSG, etc. ALLOWED AT
NO CELL PHONES, TEXT MSG, etc. ALLOWED AT

Chapter 1 ELECTROMAGNETICS OF METALS
Chapter 1 ELECTROMAGNETICS OF METALS

Alkali D Line Data
Alkali D Line Data

NMR of folded and denatured proteins
NMR of folded and denatured proteins

Protein Structure and Folding
Protein Structure and Folding

Homework-Polarizatio..
Homework-Polarizatio..

Electric Fields
Electric Fields

... If the same charge is placed nearer to the negative plate, at point B, it will again experience two forces. The force of repulsion will be reduced due to the increased distance from the positive plate. The force of attraction, however, will be increased due to the reduced distance from the negative ...
The Physics of Collective Consciousness - Philsci
The Physics of Collective Consciousness - Philsci

... they may interact with more subtle stimuli. According to my theory, this basic phenomenon works effectively when the energetic states of the constituents are close to each other. The maximal sensitivity of a system consisting of a fixed number of elements may be reached when the system builds up fro ...
UWFDM-1102 Energy and Particle Confinement Times for a Field
UWFDM-1102 Energy and Particle Confinement Times for a Field

21_published article 4
21_published article 4

Solutions of the Schrödinger equation for Dirac delta decorated
Solutions of the Schrödinger equation for Dirac delta decorated

Quantum Information Science
Quantum Information Science

Vlasov simulations of trapping and loss of auroral electrons
Vlasov simulations of trapping and loss of auroral electrons

Chapter 26 (Capacitance and Dielectrics)
Chapter 26 (Capacitance and Dielectrics)

Electrostatic PowerPoint
Electrostatic PowerPoint

The Hierarchy Problem and New Dimensions at a Millimeter
The Hierarchy Problem and New Dimensions at a Millimeter

The Photoelectric Effects: Radiation Based With Atomic Model
The Photoelectric Effects: Radiation Based With Atomic Model

P R L E T T E R S HYSICAL
P R L E T T E R S HYSICAL

Time-Reversal-Symmetry-Broken Quantum Spin Hall Effect
Time-Reversal-Symmetry-Broken Quantum Spin Hall Effect

Ab initio simulation of charged slabs at constant chemical potential
Ab initio simulation of charged slabs at constant chemical potential

< 1 ... 138 139 140 141 142 143 144 145 146 ... 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