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Angular momentum operator
Angular momentum operator

ppt - Harvard Condensed Matter Theory group
ppt - Harvard Condensed Matter Theory group

From wave functions to quantum fields
From wave functions to quantum fields

Spin-transfer Torque and Topological Changes of Magnetic Textures
Spin-transfer Torque and Topological Changes of Magnetic Textures

Influence of the Magnetic Field on the Effective Mass and the
Influence of the Magnetic Field on the Effective Mass and the

... measured to observe α. The beat patterns of the SdH oscillation imply that two different frequency terms exist. This means that the concentrations of spin-up and -down electrons are different in the channel. From the temperature dependence of the oscillation amplitude, one can also estimate the effe ...
Lecture 12
Lecture 12

... • Define the x-y axes. Typically, the x-axis is defined along the line of impact and the y-axis is in the plane of contact perpendicular to the x-axis. • For both central and oblique impact problems, the following equations apply along the line of impact (x-dir.):  m(vx)1 =  m(vx)2 and e = [(vBx)2 ...
berezinskii-kosterlitz-thouless transition and the haldane conjecture
berezinskii-kosterlitz-thouless transition and the haldane conjecture

... To make this point more explicit, we estimate the energy that it takes to implement one V or one AV in an otherwise smooth configuration. We do so in a simplified scheme of a quasi-continuous plane: close to the transition this can be justified since ξ (the relevant scale) is much larger than the la ...
r2 - SIUE
r2 - SIUE

An Integration of General Relativity and Relativistic Quantum
An Integration of General Relativity and Relativistic Quantum

... operator L in linear vector space of fundamental operators, L = aiLi , i = 1, 2, … with closure L|a> = |b> Assume that the Li form a non-commutative algebra of fundamental actions [Li , Lj] = cijk Lk. and which is (normally) a Lie algebra. Thus |a> must be a representation space of this algebra wher ...
Spin
Spin

... Nuclear magnetic resonance, or NMR as it is abbreviated by scientists, is a phenomenon which occurs when the nuclei of certain atoms are immersed in a static magnetic field and exposed to an oscillating electromagnetic field. Some nuclei experience this phenomenon, and others do not, dependent upon ...
Quantum Criticality - Subir Sachdev
Quantum Criticality - Subir Sachdev

Majorana Fermions - Physics | Oregon State University
Majorana Fermions - Physics | Oregon State University

... • None of the standard model fermions (with the possible exception of the neutrino) are their own antiparticles. • As such, they are sometimes called Dirac fermions in opposition to Majorana fermions. ...
Spin Azimuthal Asymmetries inSemi-Inclusive DIS at
Spin Azimuthal Asymmetries inSemi-Inclusive DIS at

Quantum critical point and spin fluctuations in the lower
Quantum critical point and spin fluctuations in the lower

Quantum Numbers - Chemwiki
Quantum Numbers - Chemwiki

... Pauli Exclusion Principle: In 1926, Wolfgang Pauli discovered that a set of quantum numbers is specific to a certain electron. That is, no two electrons can have the same values for n, l, ml, and ms. Although the first three quantum numbers identify a specific orbital and may have the same values, t ...
Chemical Physics High-spin-low-spin transitions in Fe(II) complexes
Chemical Physics High-spin-low-spin transitions in Fe(II) complexes

Doublet Fine Structure and the Spinning Electron
Doublet Fine Structure and the Spinning Electron

... From t he very earli est obser va ti ons of spectra l series it has been known t hat each member of certain genera l t y pes of series shows fine st ruc t ur e while t hose of others do not. Each member of some of t he series in the alkali metals, for example, is a close doublet (see F ig. 1.9), whe ...
Spin and uncertainty in the interpretation of quantum mechanics
Spin and uncertainty in the interpretation of quantum mechanics

Magnetic order in nuclear spin two-dimensional lattices due to electron–electron interactions
Magnetic order in nuclear spin two-dimensional lattices due to electron–electron interactions

CH437 CLASS 7
CH437 CLASS 7

... external magnetic field Bo are subjected to a radiofrequency field B1 (frequency ), applied in the x direction, with Bo in the z direction. At 7.04 T, E calculated from equation (4) has values (in the millijoules per mole region) corresponding to frequencies (since E = h) of only 300 MHz for 1H ...
Time reversal (reversal of motion)
Time reversal (reversal of motion)

... The probability current corresponding to the wave function R(r)Ylm seems to turn clockwise when looked at from the direction of the positive z-axis and m > 0. The probability current of the corresponding time reversed state on the other hand turns counterclockwise because m changes its sign under th ...
1 The Paramagnet to Ferromagnet Phase Transition
1 The Paramagnet to Ferromagnet Phase Transition

... state. However, when 4J/kT = 2, i.e., at a temperature T = 2J/k, then the two curves are y =< s > and y = tanh(2 < s >) (dotted curve). These curves also cross at < s >= ±0.96. There are ferromagnetic solutions, solutions with non-zero < s > at this temperature: the Ising model is in the ferromagnet ...
Chapter 2 Atomic structure and spectra
Chapter 2 Atomic structure and spectra

... where φj (qi ) = Rnj j (ri )Yj mj (θi , ϕi )σmsj represents a spin orbital with σmsj being the spin part of the orbital, either α for msj = 1/2 or β for msj = −1/2 . The electron wave function in Equation (2.16) gives the occupation of the atomic orbitals and represents a given electron configurat ...
Is the moon there when nobody looks?
Is the moon there when nobody looks?

Magnetic Excitations of Stripes near a Quantum Critical Point
Magnetic Excitations of Stripes near a Quantum Critical Point

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Spin (physics)

In quantum mechanics and particle physics, spin is an intrinsic form of angular momentum carried by elementary particles, composite particles (hadrons), and atomic nuclei.Spin is one of two types of angular momentum in quantum mechanics, the other being orbital angular momentum. The orbital angular momentum operator is the quantum-mechanical counterpart to the classical notion of angular momentum: it arises when a particle executes a rotating or twisting trajectory (such as when an electron orbits a nucleus). The existence of spin angular momentum is inferred from experiments, such as the Stern–Gerlach experiment, in which particles are observed to possess angular momentum that cannot be accounted for by orbital angular momentum alone.In some ways, spin is like a vector quantity; it has a definite magnitude, and it has a ""direction"" (but quantization makes this ""direction"" different from the direction of an ordinary vector). All elementary particles of a given kind have the same magnitude of spin angular momentum, which is indicated by assigning the particle a spin quantum number.The SI unit of spin is the joule-second, just as with classical angular momentum. In practice, however, it is written as a multiple of the reduced Planck constant ħ, usually in natural units, where the ħ is omitted, resulting in a unitless number. Spin quantum numbers are unitless numbers by definition.When combined with the spin-statistics theorem, the spin of electrons results in the Pauli exclusion principle, which in turn underlies the periodic table of chemical elements.Wolfgang Pauli was the first to propose the concept of spin, but he did not name it. In 1925, Ralph Kronig, George Uhlenbeck and Samuel Goudsmit at Leiden University suggested a physical interpretation of particles spinning around their own axis. The mathematical theory was worked out in depth by Pauli in 1927. When Paul Dirac derived his relativistic quantum mechanics in 1928, electron spin was an essential part of it.
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