• 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
ReviewWavesO
ReviewWavesO

PDF version
PDF version

Renormalization of the Drude Conductivity by the Electron-Phonon Interaction
Renormalization of the Drude Conductivity by the Electron-Phonon Interaction

Paper
Paper

... field gradients up to a few G=cm can be applied with external coils, and calibrated using Stern-Gerlach separation of the different spin states after release from the trap. The gradient is applied along the x direction, which is the weakest axis of the crossed dipole trap. Absorptive imaging of the ...
Ab initio theory of ferromagnetic transition metals and alloys under
Ab initio theory of ferromagnetic transition metals and alloys under

Experimental nonlocal and surreal Bohmian trajectories
Experimental nonlocal and surreal Bohmian trajectories

Lecture Notes 09: Electrostatic Fields In Matter, Dielectric Materials and Their Properties
Lecture Notes 09: Electrostatic Fields In Matter, Dielectric Materials and Their Properties

... It can be seen that atomic polarizability  has dependence on outer-most shell/valence electron! (i.e. the least tightly bound electron to nucleus - due to screening effects of inner shell electrons). It is (certainly) possible to obtain a theoretical relation - i.e. a theoretical “pre-diction” (tec ...
Different Alfvén wave acceleration processes of electrons - HAL-Insu
Different Alfvén wave acceleration processes of electrons - HAL-Insu

Physics can only be
Physics can only be

1. An electron situated near another electron would feel an attractive
1. An electron situated near another electron would feel an attractive

... at infinity can a 1 µC charge be placed so that there will be no net electrostatic force on it? → At one point on the x-axis to the left of the positive charge. At some point off the x-axis either above or below. At one point between the two charges. At one point on the x-axis to the right of the ne ...
Postprint
Postprint

... (or equivalently of a comb of coherent odd harmonic frequencies (2q + 1)ω: H2q+1 ). Under these conditions, the photoelectron spectrum consists of equidistant lines separated by 2ω that are associated to one-photon ionization of the target by each harmonic. In-between these lines are sidebands assoc ...
Chapter 10 - From CRTs to CROs and TVs
Chapter 10 - From CRTs to CROs and TVs

... Low pressure: A functional CRT must have its glass tube evacuated to a very low gas pressure, preferably close to vacuum. This is because the cathode and anode are separated by quite a large distance inside the tube. The low pressure inside the tube ensures minimal collisions between the air molecul ...
Plasma Electrodynamics and Applications—A. Bers, A. K. Ram
Plasma Electrodynamics and Applications—A. Bers, A. K. Ram

... plasma density through an ad-hoc equation of state.1 Satisfactory results are sometimes obtained from this simple model by appropriately choosing (a posteriori) the free parameter in the equation of state. However, fundamentally, this approach suffers from the constraint that perturbations in pressu ...
On the Use of the Geometric Mean in FDTD Near-to-Far
On the Use of the Geometric Mean in FDTD Near-to-Far

... In this paper, we are interested in using the time-domain nearfields to determine the harmonic far-fields at a few discrete frequencies. This approach allows one to easily calculate the scattering in any direction. However, alternate transformations exist which permit the direct calculation of the t ...
Condensed Matter Approaches to Quantum Gases
Condensed Matter Approaches to Quantum Gases

... The discovery of Bose-Einstein condensation (BEC) in dilute atomic gases of Rb [1], Na [2], and Li [3] in magnetic traps has stimulated an enormous revival of the interest in macroscopic quantum behavior of dilute gases at low temperature. Up to this discovery the main emphasis had been on the devel ...
Low-field microwave absorption in pulsed lased deposited FeSi thin films
Low-field microwave absorption in pulsed lased deposited FeSi thin films

... The LFA measurements were made at 9.4 GHz (X-band) on pulse laser deposited (PLD) polycrystalline B20 cubic structure FeSi thin film grown on Si (111) substrate. PLD is regarded as a powerful tool for thin film growth. The LFA properties of the films were investigated as a function of DC field, tem ...
Negative-energy waves in a plasma with structured magnetic fields
Negative-energy waves in a plasma with structured magnetic fields

Reduction of Sheath Potential and Dust Ion
Reduction of Sheath Potential and Dust Ion

... where the electric field at the plate becomes zero, the stationary oscillation in a potential distribution appears. This oscillation is confirmed to be a dust ion-acoustic wave, where the dust charge determines the wavelength and electrons do not contribute to the oscillation except for the vicinity ...
Physics
Physics

IBM Josephson junction qubit
IBM Josephson junction qubit

The Relativistic Electrodynamics Turbine. Experimentum
The Relativistic Electrodynamics Turbine. Experimentum

4 Measurements
4 Measurements

... field strength amplitudes is a constant, Z0, which is known as the characteristic impedance of free space1 and is about 377 Ω (or 120 Ω). Thus, in the far field, the power density, S, in free space is given by the following non-vector ...
Exploring the Earth`s Magnetic Field
Exploring the Earth`s Magnetic Field

... What are magnetic fields? In physical science, a "field of force " is a region or space in which an object can cause a push or pull. This field extends infinitely in all directions but gets weaker as you get farther from the source of the field. Magnetic lines of force show the strength and directio ...
Dynamical Franz-Keldysh effect in the optical and terahertz regime
Dynamical Franz-Keldysh effect in the optical and terahertz regime

One-dimensional theory of the quantum Hall system
One-dimensional theory of the quantum Hall system

< 1 ... 80 81 82 83 84 85 86 87 88 ... 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