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A critique of recent semi-classical spin-half quantum plasma theories
A critique of recent semi-classical spin-half quantum plasma theories

... orbit theory”. Specifically, if the time rate of change of the fields is measured by the frequency ω and the spatial scales are represented by the wave number k , drift orbit theory may be used when ρ∗ = Max[kρe , ωωce ] ≪ 1. Here, c⊥ is the “peculiar velocity” of the electron’s Larmor gyro motion. ...
Charge accumulation in DC cables
Charge accumulation in DC cables

Nuclear Spin Ferromagnetic transition in a 2DEG Pascal Simon
Nuclear Spin Ferromagnetic transition in a 2DEG Pascal Simon

... Central issue for quantum computing: decoherence of spin qubit Sources of spin decay in GaAs quantum dots: • spin-orbit interaction (bulk & structure): couples charge fluctuations with spin  spin-phonon interaction, but this is weak in quantum dots (Khaetskii&Nazarov, PRB’00) ...
The use of Electron Paramagnetic Resonance (EPR) in the probing
The use of Electron Paramagnetic Resonance (EPR) in the probing

Question Bank Physics Class 12
Question Bank Physics Class 12

Speed of light - should be measured once again
Speed of light - should be measured once again

... This quantity, sometimes called Maxwell’s constant, enables one to express the total force of electromagnetic origin FEM = FE + FM in a compact form FEM = FE (1  v2 / b2 ), ...
Chapter 23 Electric Fields. Solutions of Home Work Problems
Chapter 23 Electric Fields. Solutions of Home Work Problems

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162-02-04-2015-chapter-28

motional EMF
motional EMF

Spring 2016 Final Exam Review: Physics 1P, Mr. Traeger
Spring 2016 Final Exam Review: Physics 1P, Mr. Traeger

... look like around positive and negative charges? What direction do electric field lines always point in? What is lightning and how is it produced? What is electric shielding and why does charge build up on the outside of objects, but not in them? How does a positive test charge behave when forced tow ...
Learning station IX : Spin and its applications - Quantum Spin-Off
Learning station IX : Spin and its applications - Quantum Spin-Off

... the down state at the same time . This means that we can actually store more information in a spin than we could in a simple 1 or 0. The field of electronics in which spin is also used is called spintronics. The nobel prize in physics of 2007 was awarded for the discovery of an effect known as giant ...
Eðlisfræði 2, vor 2007
Eðlisfræði 2, vor 2007

Chapter 2: Sensor Characteristics and Physical Effects
Chapter 2: Sensor Characteristics and Physical Effects

... stimulus. A transducer is a device that converts one form on energy into another. Generally, a sensing or sensitive layer/medium directly responds to the external stimulus, while the transducer converts the response into an external measurable quantity. As distinct from detectors, sensors are employ ...
Magneto-Electro-V iscoelastic Torsional Waves in
Magneto-Electro-V iscoelastic Torsional Waves in

... the solid body, give rise to the coupled field of magneto-elasticity. Since electric currents also give rise to magnetic field and vice-versa, the combined effect is also sometimes known as magnetoelectro-elasticity. It is evident that since many component fields are interacting, a large number of u ...
Chapter 21: Electric Charge and Electric Field
Chapter 21: Electric Charge and Electric Field

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Electrostatics PP

Gauss`s law and examples with insulators
Gauss`s law and examples with insulators

... A. What is the electric field from an infinite plane sheet of positive charge with uniform surface charge density σ? Symmetry in this problem dictates that the electric field must be perpendicular to the plan and point away from its positively charged surface. Also, the electric field can only depen ...
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lecture chapter 23

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Electric Potential

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Electric Potential Practice Problems

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CH22-revision-lecture - University of Southampton

Solar cycle dependence of quiet-time magnetospheric currents
Solar cycle dependence of quiet-time magnetospheric currents

... calculated. Results are presented in Fig. 2 as plus signs with error bars. This quantity shows major solar cycle dependence. Large annual means up to 17 nT are obtained during the years 2001 through 2005; subsequently they decay to 2 nT in 2009. An interpretation in terms of magnetospheric currents ...
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On quantization of gravitational waves

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... 1. Power up the DC power supply and set acceleration potential U = 300 V. Thermionic emission starts after warming up for a few minutes. 2. Optimize focusing of the electron beam by varying the voltage at the Wehnelt-cylinder from 0 … 10 V until it leads to a narrow, well defined beam with clear edg ...
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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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