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Topic 10: Fields
Topic 10: Fields

PHYS13071 Assessment 2012
PHYS13071 Assessment 2012

... Although the foundation of quantum theory was developed in the 1920s, the last decade has seen years of great advances in quantum technology, especially in nanotechnology. According to the “Moore’s Law”, the number of transistors on computer chips, and hence their computational speed and memory capa ...
Electric Fields
Electric Fields

Thursday, Sept. 8, 2011
Thursday, Sept. 8, 2011

Nonlocal Photorefractive Screening from Hot Electron Velocity Saturation in Semiconductors
Nonlocal Photorefractive Screening from Hot Electron Velocity Saturation in Semiconductors

... the signal-to-noise limit of the four-wave mixing experiment. At this reduced modulation index, the phase shift was again measured to be approximately sin"f# ! 0.9, which is consistent with the high-modulation value. It has also been pointed out that small modulation results are semiquantitatively v ...
Lecture16
Lecture16

Real-World Quantum Measurements
Real-World Quantum Measurements

The Electric Field
The Electric Field

... Objects carrying charges of opposite signs attract each other; Objects carrying charges of the same sign repel each other Positive, the charge acquired by a glass rod when is rubbed with a piece of silk, (Franklin criteria), then electrons are transferred to silk. The piece of silk acquires the same ...
the motion of charged particles in a random magnetic field
the motion of charged particles in a random magnetic field

Electric bi
Electric bi

Chapter 21: Electric Charge and Electric Field
Chapter 21: Electric Charge and Electric Field

The Schrödinger Equation
The Schrödinger Equation

... But one thing has not been seen Just what does psi really mean” From: Walter Hückel, translated by Felix Bloch The Schrödinger equation allows to calculate analytically [exactly] quantum problems, but it does not reveal the nature of Ψ. Schrödinger called it “field scalar”. “Shut up and Calculate !” ...
PHZ7427: Spring 2014 Josephson effect D. L. Maslov 392-0513 Rm. NPB2114
PHZ7427: Spring 2014 Josephson effect D. L. Maslov 392-0513 Rm. NPB2114

Dual approaches for defects condensation
Dual approaches for defects condensation

... whole space these two methods are dual equivalent prescriptions to obtain an effective theory for the phase where the defects (like monopoles or vortices) are completely condensed, starting from the fundamental theory defined in the normal phase where the defects are diluted. Keywords: Topological d ...
Lectronic Plates
Lectronic Plates

... 6. What is the strongest electric field you can create in the sim with the battery connected? a. Record the value:____________________ b. Comment on each parameter in the configuration, indicating whether it should be at a maximum, minimum, or if it’s irrelevant: battery voltage (V), plate area (A), ...
Chapter 17
Chapter 17

... – Remember that stated there was an attractive force between all objects depending on mass and separation. ...
EM_Course_Module_4 - University of Illinois at Urbana
EM_Course_Module_4 - University of Illinois at Urbana

Electric Potential
Electric Potential

Adobe Acrobat file () - Wayne State University Physics and
Adobe Acrobat file () - Wayne State University Physics and

Quantum-Phase-Field Concept of Matter: Emergent
Quantum-Phase-Field Concept of Matter: Emergent

... where no length scale is given. Mesoscopic in this context means ‘large compared to elementary particles or atoms’ and ‘small compared to the size of the body’. Then, the scale of a typical pattern is treated emergent from interactions between different elements of the body under investigation. The ...
$doc.title

... (d) Find the most general solution to this differential equation which satisfies the above two properties. ˆt is often called the “Evolution operator” or the “Propagator”. In principle, we Aside: U can always solve the Schrödinger equation by simply exponentiating − ni tÊ; acting with ˆt on a given ...
MU08-CHAPTER4.doc
MU08-CHAPTER4.doc

Lab 3: Electric Fields II
Lab 3: Electric Fields II

27.8. Model: The rods are thin. Assume that the charge lies along a
27.8. Model: The rods are thin. Assume that the charge lies along a

DC TRANSFORMER AND DC JOSEPHSON(-LIKE) EFFECTS IN QUANTUM HALL BILAYERS
DC TRANSFORMER AND DC JOSEPHSON(-LIKE) EFFECTS IN QUANTUM HALL BILAYERS

< 1 ... 349 350 351 352 353 354 355 356 357 ... 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).
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