• 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
CCR 7: Derivation of the Boltzmann Distribution
CCR 7: Derivation of the Boltzmann Distribution

The quantum system - Università degli Studi dell`Insubria
The quantum system - Università degli Studi dell`Insubria

... which form the vector operator p$  p$x , p$y . Both components of the linear momentum operator commute with the Hamiltonian [ H$, p$x ]  [ H$, p$y ]  0 and then we find again that the linear momentum is a constant of motion. This mathematical result has again a deep physical significance: the lin ...
Magnetoresistance.
Magnetoresistance.

... orbital angular momentum. Orbital angular momentum is the qunatum number that changes in the quantum Hall effect. When polycrystalline samples (or arbitrary angles of the applied magnetic field to the atomic planes) are used in the Hall experiment it is necessary for electrons to cross from one atom ...
Spin-current and other unusual phases in magnetized triangular lattice antiferromagnets
Spin-current and other unusual phases in magnetized triangular lattice antiferromagnets

... been proposed that the plateaus are Wigner crystals of triplets [14–16]. There exists a spin model which is derived from the Shastry-Sutherland Hamiltonian [17] for which the plateaus are demonstrated to originate from such ordered states. However, in this model there are plateaus at 1#4, 1#2, and 3 ...
Sufficient Conditions for Efficient Classical Simulation of Quantum
Sufficient Conditions for Efficient Classical Simulation of Quantum

[tex110] Occupation number fluctuations
[tex110] Occupation number fluctuations

... ...
1 Invariance and quantization of charges and currents
1 Invariance and quantization of charges and currents

Whittaker Functions and Quantum Groups
Whittaker Functions and Quantum Groups

... of vertices that there exists a vertex ST such that the Yang-Baxter equation is true in the sense that the following two partition functions are equal: ...
2. The HameroffŁs gap junction tunneling
2. The HameroffŁs gap junction tunneling

The next stage: quantum game theory
The next stage: quantum game theory

Frustrated Quantum Magnetism with Laser-Dressed Rydberg Atoms
Frustrated Quantum Magnetism with Laser-Dressed Rydberg Atoms

... Rb atoms and choose |g+ i ≡ |52 S1/2 , F = 2, mF = 2i and |g- i ≡ |52 S1/2 , F = 1, mF = 1i as our spin-1/2 [see Fig. 1(b)]. Interactions between these effective spin states are induced by admixing highly lying Rydberg states to the atomic ground states with laser light, where van der Waals (vdW) in ...
Angular momentum operator
Angular momentum operator

Quantum entanglement between the electron clouds of nucleic acids
Quantum entanglement between the electron clouds of nucleic acids

PDF
PDF

... in three different “states”: it can be bound to its system, unbound, or in the ground state (the state such that information contained in the carrier is not relevant anymore.) Carriers become unbound when a measurement is made on their associated systems. They are then free to interact with other sy ...
Detailing Coherent, Minimum Uncertainty States of Gravitons, as
Detailing Coherent, Minimum Uncertainty States of Gravitons, as

... author is convinced after trial and error that the standard which should be used is that of talking of information, in the Shannon sense, for entropy, and to find ways to make a relationship between quantum computing operations, and Shannon information. Making the identification of entropy as being ...
Electronic Properties of Coupled Quantum Rings in the Presence of
Electronic Properties of Coupled Quantum Rings in the Presence of

PDF
PDF

... experiment can be used to eliminate the modulus π uncertainty. Specifically, if one applies a dc magnetic field parallel to the RF field, it leads to a new oscillation (in the population of either level) at the fundamental frequency, with exactly the same phase as that of the driving field. In the e ...
functions and (so-called px- and py-orbitals) are linear combinations
functions and (so-called px- and py-orbitals) are linear combinations

Scientific discoveries limit our knowledge
Scientific discoveries limit our knowledge

Spontaneous Symmetry Breaking in Non Abelian Gauge Theories
Spontaneous Symmetry Breaking in Non Abelian Gauge Theories

... We can take a similar Lagrangian for the scalar field as above L = |∂φ|2 − V (|φ|2 ) (where Lorentz and SU (N ) index sums are implied) which has the required invariance. To promote the symmetry to a local symmetry, we must replace the derivatives with covariant derivatives Dµ = ∂µ − igAµ . The gaug ...
Path-Integral Molecular Dynamics at Thermal Equilibrium
Path-Integral Molecular Dynamics at Thermal Equilibrium

TQFTs - UCSB Math Department
TQFTs - UCSB Math Department

... Bordism here is called a smooth manifold triad. A cobordism from Y1 to Y2 there is defined as a 5-tuple (X; ∂1 X, ∂2 X; h1 , h2 ), where (X; ∂1 X, ∂2 X) is a smooth triad and hi : ∂i X → Yi , i = 1, 2 are diffeomorphisms. This definition leads to a category of manifolds, which are often called the co ...
Radiative cascade of highly excited hydrogen atoms in strong magnetic... Türker Topçu and Francis Robicheaux 兲
Radiative cascade of highly excited hydrogen atoms in strong magnetic... Türker Topçu and Francis Robicheaux 兲

... Formation of highly excited antihydrogen atoms have been reported by two experimental groups where cold antiprotons are merged with a cold trapped positron plasma at roughly 关1兴 16 K and 关2,3兴 4 K in magnetic fields of about 3 and 5.4 T, respectively. The goal is to perform Lorentz and CPT violation ...
Curriculum Vitae Irinel Chiorescu
Curriculum Vitae Irinel Chiorescu

... direction I developed at FSU is focusing on quantum coherence and it involves studies of spin dynamics in diluted spin systems and molecular magnets. The research program benefited from an Alfred P. Sloan Research Fellowship and a NSF Career award, now continued with a regular NSF grant. This goal i ...
10 Supersymmetric gauge dynamics: N = 1 10.1 Confinement and
10 Supersymmetric gauge dynamics: N = 1 10.1 Confinement and

... If confinement occurs, we would expect a linear potential between the two quarks. Indeed, in an unconfined theory, the electric flux is uniformly distributed over a sphere surrounding a charge, and falls-o↵ as 1/r2 . In a confining theory with flux tubes, the flux tube has a fixed cross-sectional ar ...
< 1 ... 145 146 147 148 149 150 151 152 153 ... 503 >

Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
  • studyres.com © 2025
  • DMCA
  • Privacy
  • Terms
  • Report