• 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
Project
Project

... cosine of the angle= -0.8944271909999159 The value of the x component of the Electric field at point: P1 due to charge point #: 2 is -48.25 sine of the angle= 0.4472135954999579 The value of the y component of the Electric field at point: P1 due to charge point #: 2 is 24.12 The magnitude of the re ...
magnetic field - iGCSE Science Courses
magnetic field - iGCSE Science Courses

... generated, and a current flows. The slip rings keep the coil in contact with the brushes throughout the rotation, and as a result the current flows in ...
EE3321 ELECTROMAGENTIC FIELD THEORY
EE3321 ELECTROMAGENTIC FIELD THEORY

+1 +2 d
+1 +2 d

Electronic transport for armchair graphene nanoribbons with a
Electronic transport for armchair graphene nanoribbons with a

Wick calculus
Wick calculus

... free quantum field. 共The reader who wishes a quick reminder of some basic quantum field-theoretical concepts may find comfort in Appendix A兲. In addition to the usual concept of quantizing by promoting fields to operators, modern quantum field theory uses functional integrals as basic objects. In th ...
Ch 28 assigned solutions
Ch 28 assigned solutions

... Adding second equation to this equation, 2q1  4q  q1  2q That is, q1  2q, q2  q, and q3  3q. ...
INTRINSIC SPIN
INTRINSIC SPIN

Chapter 8 Path Integrals in Statistical Mechanics
Chapter 8 Path Integrals in Statistical Mechanics

Name: Roll No: Final Exam: Part A List of Physical Constants
Name: Roll No: Final Exam: Part A List of Physical Constants

... find the torque τ exerted on the charged ring due to the changing magnetic field. [7 marks] ...
CHAPTER 30 Magnetic Induction
CHAPTER 30 Magnetic Induction

... 27 ∙∙ A bar magnet moves with constant velocity along the axis of a loop as shown in Figure 30-34. (a) Make a qualitative graph of the flux φm through the loop as a function of time. Indicate the time t1 when the magnet is halfway through the loop. (b) Sketch a graph of the current I in the loop ver ...
A Dynamical Theory of the Electromagnetic Field - Free-Energy-Info
A Dynamical Theory of the Electromagnetic Field - Free-Energy-Info

Some Solutions of the 3D Laplace Equation in a Layer with
Some Solutions of the 3D Laplace Equation in a Layer with

What`s new with NOON States
What`s new with NOON States

Check for Understanding
Check for Understanding

Modeling Domain Wall Dynamics in Thin Magnetic Strips With
Modeling Domain Wall Dynamics in Thin Magnetic Strips With

Potential - Chabot College
Potential - Chabot College

Paired Hall states
Paired Hall states

... detail. We argue that it leads unambiguously to pairing in the p-wave for weak coupling (that is, small deviations from fermi statistics at zero external field.) Unfortunately, the most interesting case v 1/2 is far from this limit, and other approaches must be used. Fortunately, the pairing analysi ...
Quiz LEVEL 1 1.The circumstance under which line charge can be
Quiz LEVEL 1 1.The circumstance under which line charge can be

Evidence for Two Different Solid Phases of Two-Dimensional Electrons in... * Z. H. Wang, Yong P. Chen, R. M. Lewis,
Evidence for Two Different Solid Phases of Two-Dimensional Electrons in... * Z. H. Wang, Yong P. Chen, R. M. Lewis,

... It has been thought that correlations responsible for the FQHE can still be relevant [22 –25] even in the HBIP. More specifically, theories [23–25] have considered different types of ‘‘correlated’’ WSs (m CWS) made of ‘‘composite fermions’’ or ‘‘composite bosons,’’ the quasiparticles [electrons boun ...
Capacitance
Capacitance

the electric field - Haiku for Ignatius
the electric field - Haiku for Ignatius

Chapter 4 MHD Equilibrium and Stability
Chapter 4 MHD Equilibrium and Stability

Slater decomposition of fractional quantum Hall states
Slater decomposition of fractional quantum Hall states

... Tsui, Stormer and Gossard [TSG82], but because of its intrinsically strongly correlated nature, is not yet completely understood. Among the relevant questions, it is not clear why the celebrated Laughlin’s ansatz is such a good approximation for exact ground states of the system. From a more mathema ...
Unit C Chapter 1 Lesson 2 - Lacombe Composite High School
Unit C Chapter 1 Lesson 2 - Lacombe Composite High School

< 1 ... 181 182 183 184 185 186 187 188 189 ... 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