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wavefunction (63) obtained by applying Dirac`s factor
wavefunction (63) obtained by applying Dirac`s factor

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- Free Documents

Spontaneous Formation of Magnetic Moments and Dephasing in Two-Dimensional Disordered Systems
Spontaneous Formation of Magnetic Moments and Dephasing in Two-Dimensional Disordered Systems

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Fysiikan seminaarit -haku Oulun yliopisto | Fysiikan seminaarit

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The g factor of conduction electrons in aluminium : calculation

... The conduction electron spin resonance ( CESR) of aluminium has been studied extensively over the last few years. The main parameters of the resonance (y factor and linewidth) show a dependence with temperature and also with the frequency of the spectrometer which is not understood at present. In th ...
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Quantum Correlated Interstitials and the Hall Resistivity of the

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179 tut Tunneling - University of Maine Physics Education

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A study of the effects of electromagnetic fields on the growth and

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Enhancement of Tunneling from a Correlated 2D Electron System

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Chapter 3: The Structure of Crystalline Solids

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Impact of Spin-Orbit Coupling on Quantum Hall

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Chapter 11 Coordination Chemistry III: Electronic Spectra

... The spin multiplicity is the same as the # of microstates. Each terms has different energies; they represent three states with different degrees of electron-electron interactions. Which term has the lowest energy. This can be done by using two of Hund’s rules. 1. The ground term (term of lowest ener ...
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Mixed quantum and classical processes in strong fields

Atomic Orbitals Lab - North Carolina High School Computational
Atomic Orbitals Lab - North Carolina High School Computational

... electrons are found in fixed and quantifiable levels called orbits, or, in older terminology, shells. There are specific numbers of electrons that can be found in each orbit – 2 for the first orbit, 8 for the second, and so forth. The Bohr model is very useful for predicting the behaviors of a numbe ...
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atomic spectroscopy 2005

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Ferromagnetism



Not to be confused with Ferrimagnetism; for an overview see Magnetism.Ferromagnetism is the basic mechanism by which certain materials (such as iron) form permanent magnets, or are attracted to magnets. In physics, several different types of magnetism are distinguished. Ferromagnetism (including ferrimagnetism) is the strongest type: it is the only one that typically creates forces strong enough to be felt, and is responsible for the common phenomena of magnetism in magnets encountered in everyday life. Substances respond weakly to magnetic fields with three other types of magnetism, paramagnetism, diamagnetism, and antiferromagnetism, but the forces are usually so weak that they can only be detected by sensitive instruments in a laboratory. An everyday example of ferromagnetism is a refrigerator magnet used to hold notes on a refrigerator door. The attraction between a magnet and ferromagnetic material is ""the quality of magnetism first apparent to the ancient world, and to us today"".Permanent magnets (materials that can be magnetized by an external magnetic field and remain magnetized after the external field is removed) are either ferromagnetic or ferrimagnetic, as are other materials that are noticeably attracted to them. Only a few substances are ferromagnetic. The common ones are iron, nickel, cobalt and most of their alloys, some compounds of rare earth metals, and a few naturally-occurring minerals such as lodestone.Ferromagnetism is very important in industry and modern technology, and is the basis for many electrical and electromechanical devices such as electromagnets, electric motors, generators, transformers, and magnetic storage such as tape recorders, and hard disks.
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