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Characterization of the phase transition in coper-gold alloys by X
Characterization of the phase transition in coper-gold alloys by X

Magnetic properties of materials Part 2. Types of magnetism
Magnetic properties of materials Part 2. Types of magnetism

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Characterization of Products from Oxalato Complexes

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Chapter 14 - WebAssign

... The magnitude of Δ can also influence the number of unpaired electrons on the metal, which is usually designated by the spin of the atom, ion, or molecule. The spin of a species is the sum of the individual electron spins. If there are no unpaired electrons, then there is no spin because the sum of ...
Ground state in systems with dipole interaction
Ground state in systems with dipole interaction

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Driven coherent oscillations of a single electron spin in a quantum dot

... probe experiments19,20. The only missing ingredient for universal quantum computation with spins in dots remained the demonstration of driven coherent spin rotations (Rabi oscillations) of a single electron spin. The most commonly used technique for inducing spin flips is electron spin resonance (ES ...
Chem 110 Fall 2004 Exam I Key Information You May Need: 100 cm
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Processing quantum information in diamond



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8 Magnetism - ITP, TU Berlin

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Magnetostriction vs. Magnetoelastic Effects

... all ferromagnetic materials. It couples elastic, electric, magnetic and in some situations also thermal fields and is of great industrial interest for use in sensors, actuators, adaptive or functional structures, robotics, transducers and MEMS. A magnetostrictive material develops large mechanical d ...
Small molecule Crystallography at the Indian Institute of Science
Small molecule Crystallography at the Indian Institute of Science

... The research program for Chemical Sciences Division essentially involves structure determination of inorganic systems ranging from metal hydrides, Cu I and Cu II complexes, Calixarenes and Phosphazenes and related metal complexes, organic frameworks depicting biological activity like for example Ott ...
Small molecule Crystallography at the Indian Institute of Science
Small molecule Crystallography at the Indian Institute of Science

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Spin and charge density waves around ruthenium impurity in -iron

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1 CHAPTER 12 PROPERTIES OF MAGNETIC MATERIALS 12.1

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1 CHAPTER 12 PROPERTIES OF MAGNETIC MATERIALS 12.1

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John T. Yim, Michael Keidar, and Iain D. Boyd

... – no measurements of sputter yield exist for BN at Xe+ energies below 100 eV – this region of the sputter yield profile has a large influence on Hall thruster erosion ...
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Chapter 1-Crystal Properties_M A Islam_Lecture 1

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Computer Assisted Physics - Physik

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Chapter 5: Magnetic Systems in

... refrigerator door. This magnet likely consists of iron ions localized on sites of a lattice with conduction electrons that are free to move throughout the crystal. The iron ions each have a magnetic moment and due to a complicated interaction with each other and with the conduction electrons, they t ...
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Formation of a Surface–Sandwich Structure in Pd

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Near-band-gap photo-induced nuclear spin

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Propagation of Spin-Polarized Electrons Through Interfaces

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Geometrical frustration



In condensed matter physics, the term geometrical frustration (or in short: frustration) refers to a phenomenon, where atoms tend to stick to non-trivial positions or where, on a regular crystal lattice, conflicting inter-atomic forces (each one favoring rather simple, but different structures) lead to quite complex structures. As a consequence of the frustration in the geometry or in the forces, a plenitude of distinct ground states may result at zero temperature, and usual thermal ordering may be suppressed at higher temperatures. Much studied examples are amorphous materials, glasses, or dilute magnets.The term frustration, in the context of magnetic systems, has been introduced by Gerard Toulouse (1977). Indeed, frustrated magnetic systems had been studied even before. Early work includes a study of the Ising model on a triangular lattice with nearest-neighbor spins coupled antiferromagnetically, by G. H. Wannier, published in 1950. Related features occur in magnets with competing interactions, where both ferro- as well as antiferromagnetic couplings between pairs of spins or magnetic moments are present, with the type of interaction depending on the separation distance of the spins. In that case commensurability, such as helical spin arrangements may result, as had been discussed originally, especially, by A. Yoshimori, T. A. Kaplan, R. J. Elliott, and others, starting in 1959, to describe experimental findings on rare-earth metals. A renewed interest in such spin systems with frustrated or competing interactions arose about two decades later, beginning in the 70s of the 20th century, in the context of spin glasses and spatially modulated magnetic superstructures. In spin glasses, frustration is augmented by stochastic disorder in the interactions, as may occur, experimentally, in non-stoichiometric magnetic alloys. Carefully analyzed spin models with frustration include the Sherrington-Kirkpatrick model, describing spin glasses, and the ANNNI model, describing commensurability magnetic superstructures.
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