• Study Resource
  • Explore
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Coherent Exciton Dynamics in Semiconductor Superlattices:A Quasi
Coherent Exciton Dynamics in Semiconductor Superlattices:A Quasi

... Is the position of the photon an observable? In quantum mechanics, any observable requires a Hermitian operator 1948, Pryce obtained a photon position operator, pˆ  S a a rP  i p p  p • a =1/2 for F=E+icB ~ p1/2 as in QED to normalize • last term maintains transversality of rP(F) • but the com ...
Absence of spin liquid in non-frustrated correlated systems
Absence of spin liquid in non-frustrated correlated systems

Prediction of a quantum anomalous Hall state in Co decorated silicene
Prediction of a quantum anomalous Hall state in Co decorated silicene

`Quantum Cheshire Cat`as Simple Quantum Interference
`Quantum Cheshire Cat`as Simple Quantum Interference

Fabre de la Ripelle M. A Mathematical Structure for Nuclei
Fabre de la Ripelle M. A Mathematical Structure for Nuclei

Spin and Quantum Measurement
Spin and Quantum Measurement

The Magnetic Moments of Proton, Neutron and Electron.
The Magnetic Moments of Proton, Neutron and Electron.

Introductory helium atomic spectrum analysis
Introductory helium atomic spectrum analysis

... Fig. 1. A plot of the helium spectrum for a collection time of 10 ␮s. All the spectral lines except the last four in Table I can be observed. The data were collected using the spectrometer of Ref. 3. ...
Solid-state quantum computing using spectral holes M. S. Shahriar, P. R. Hemmer,
Solid-state quantum computing using spectral holes M. S. Shahriar, P. R. Hemmer,

Realization of a Cascaded Quantum System
Realization of a Cascaded Quantum System

Multi-component fractional quantum Hall states in graphene: S U(4
Multi-component fractional quantum Hall states in graphene: S U(4

... is much weaker than that in the lowest LL. (iii) As predicted in [14–16], no FQHE has been observed at even denominator fractions in the |n| = 1 LL. Some other observations are unexpected, however. Noteworthy is the absence of fractions such as 2 − 1/3 and 2 − 2/5, while 2 − 2/3 and 2 − 4/3 are stro ...
Slide 1 - Alice Pevyhouse
Slide 1 - Alice Pevyhouse

... collapse, suppose the core of such a star is the size of our Sun (r ≈ 7 x 105 km) with mass 2.0 times as great as the Sun, and is rotating at a frequency of 1.0 revolution every 100 days. If it were to undergo gravitational collapse to a neutron star of radius 10 km, what would its rotation frequenc ...
Identical Quantum Particles and Weak Discernibility - Philsci
Identical Quantum Particles and Weak Discernibility - Philsci

... of the mapping. The following mathematical case provides another example. The numbers 1 and −1 share all their structural properties in the structure < Z, + > (the relational structure of integers with addition, without individual names for the numbers), just like the spheres in our earlier example. ...
Easy understanding on Hanle effect No.1 atomic polarization and
Easy understanding on Hanle effect No.1 atomic polarization and

Feynman Diagrams for Beginners
Feynman Diagrams for Beginners

... particle interactions can often be calculated using a relatively simple “recipe” — Feynman diagrams. Before we turn to describing the method of Feynman diagrams, let us just specify other quantum fields that take part in the elementary particle physics interactions. All these are free fields, and in ...
Electron-electron interactions in a one-dimensional quantum
Electron-electron interactions in a one-dimensional quantum

Quantum Spin Hall Effect and their Topological Design of Devices
Quantum Spin Hall Effect and their Topological Design of Devices

... introduction of spin-up spin-down scattering,[3] which destroy the quantum spin Hall effect. In order experiment was introduced a topological Z 2 , invariant who characterizes a state as trivial or non-trivial band insulator (regardless if the state exhibits or does not exhibit a quantum spin Hall E ...
JLab 12 GeV upgrade (3) [C3]
JLab 12 GeV upgrade (3) [C3]

Document
Document

Kinetics of decay of metastable gas phase of polarized atomic
Kinetics of decay of metastable gas phase of polarized atomic

Solution of the Lindblad equation for spin helix states arXiv
Solution of the Lindblad equation for spin helix states arXiv

Hydrogen 2
Hydrogen 2

Measuring the Size of Elementary Particle Collisions
Measuring the Size of Elementary Particle Collisions

Transition Probabilities and Selection Rules
Transition Probabilities and Selection Rules

Numerical Renormalization Group methods with Matrix Product States
Numerical Renormalization Group methods with Matrix Product States

... – Most pronounced quantum effects arise at low temperature as large quantum fluctuations exist (ground states) – We assume some geometry and local interactions (cfr. Causality) such as Heisenberg model ...
< 1 ... 29 30 31 32 33 34 35 36 37 ... 94 >

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.
  • studyres.com © 2025
  • DMCA
  • Privacy
  • Terms
  • Report