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Electromagnetic radiation and steady states of hydrogen atom
Electromagnetic radiation and steady states of hydrogen atom

... Light from hydrogen atom, which is one kind of electromagnetic radiation caused by moving charged particles, is the most important data to understand the structure of the atom. Although there are numerous models to describe the electromagnetic phenomena based on quantum theory, classical electrodyna ...
Imaging electrostatically confined Dirac fermions in graphene
Imaging electrostatically confined Dirac fermions in graphene

... electrostatic gating. Electron confinement in graphene has also been induced through high magnetic fields23 and supercritical impurities24 , but these methods are unwieldy for many technological applications. An alternative approach for confining electrons in graphene relies on using electrostatic p ...
Computing Quark and Gluon Distribution Functions for Very Large
Computing Quark and Gluon Distribution Functions for Very Large

... this would be true. In any case, when ρ >> Λ2QCD , we expect that the coupling constant for strong interactions is weak, and weak coupling methods should be valid for computing the distribution functions. [4] In this paper, we will show how to set up the problem of computing the distribution functio ...
Chapter 20: Magnetic field and forces What will we learn in this
Chapter 20: Magnetic field and forces What will we learn in this

... E/B will fly trough the capacitor. Thomson’s experiment: in 1894 Sir J. J. Thomson used this method to determine the ratio e/me. He noted that it was independent of the used material, i.e., he discovered subatomic particles. Later Millikan computed e and thus the electron mass was determined. ...
PDF
PDF

... and we conclude that entangled biphotons are not generated even though both pump lasers are still producing photons. The observed photon interference in Fig. 2(b) has a measured visibility of V raw ¼ 93.3  2.0%. When the accidental counts are subtracted (removing the noise from the detectors and ot ...
Ground-state properties of the attractive one
Ground-state properties of the attractive one

... many particles N and lattice sites L. Attractive boson systems are conceptually different from repulsive bosons and attractive and/or repulsive fermions, in that such a limit cannot easily be defined as discussed later on. Nevertheless, for large but finite N and L the attractive boson system does d ...
Document
Document

... Concept of charge density: for charge Q uniformly distributed over some volume V, the charge per unit volume or volume charge density is the ratio ρ = Q / V . If an object is flat (2 dimensional) the surface charge density is the ratio of the charge Q to the surface area S: σ = Q / S . For linear, o ...
Finally, it seems clear that we will never be able to explain
Finally, it seems clear that we will never be able to explain

Cooling of a small sample of Bose atoms with accidental... Maciej Lewenstein , J. Ignacio Cirac , and Luis Santos
Cooling of a small sample of Bose atoms with accidental... Maciej Lewenstein , J. Ignacio Cirac , and Luis Santos

Lecture 5: Physics Beyond the Standard Model and Supersymmetry
Lecture 5: Physics Beyond the Standard Model and Supersymmetry

Chapter 3: Gauss` Law
Chapter 3: Gauss` Law

... A formal statement of the relation between charge and flux is known as Gauss’ law. The total electric flux emerging from an arbitrary volume equals the net charge enclosed within the volume divided by ε 0 . Gauss’ Qenclosed Law φ ≡ ∫ E ⋅ dA = ...
Phases in noncommutative quantum mechanics on (pseudo) sphere
Phases in noncommutative quantum mechanics on (pseudo) sphere

Document
Document

manuscript - University of Hertfordshire
manuscript - University of Hertfordshire

... vortex form (Fig. 3 in Ref. [4]), just like in the classical case. The quantum harmonic oscillator and its isomorphism [18], the free quantum particle [19], constitute exceptional, degenerate cases where lines of stagnation of Wigner flow occur, and not only isolated stagnation points. This is due t ...
Untitled - at www.arxiv.org.
Untitled - at www.arxiv.org.

Singularity of the time-energy uncertainty in adiabatic perturbation
Singularity of the time-energy uncertainty in adiabatic perturbation

... approaches zero, the solution of the Navier-Stokes equation gives a completely different solution from the one obtained by taking the zero viscosity to start out with. Adiabatic perturbation1 is one of the fundamental approximations used in many fields. Its classic applications include the Born-Oppe ...
Spin effects in semiconductor quantum dot structures
Spin effects in semiconductor quantum dot structures

G484 Module 2 4.2.2 Gravitational Fields a
G484 Module 2 4.2.2 Gravitational Fields a

E = mc2 m = hc λc2 = h λc h λ= mv h λ= mc
E = mc2 m = hc λc2 = h λc h λ= mv h λ= mc

Ionization of Atoms with Intense, Linearly and Circularly Polarized
Ionization of Atoms with Intense, Linearly and Circularly Polarized

... The laser used for these experiments is based on the chirped-pulse-amplification . ~ ~ ~laser systems technique and has been described in detail e l ~ e w h e r e CPA allow the production of high-power, ultrashort pulses in solid-state lasing media.6 A laser pulse from a mode-locked oscillator is fr ...
Fock Spaces - Institut Camille Jordan
Fock Spaces - Institut Camille Jordan

... In the case of the anticommutation relations, one does not need to rewrite them, for b(x) and b∗ (x) are always bounded operators (as we shall prove later). But the concrete realisation of the C.A.R. is always made through the antisymmetric Fock spaces. The importance of Fock space comes from the fa ...
Three-dimensional electromagnetic breathers in carbon
Three-dimensional electromagnetic breathers in carbon

Precision spectroscopy with two correlated atoms
Precision spectroscopy with two correlated atoms

8.4 Motion of Charged Particles in Magnetic Fields
8.4 Motion of Charged Particles in Magnetic Fields

... between the objects, which transmits the force. To develop a more accurate concept of force, we need to talk about it in terms of fields. We know that all objects are made of atoms interacting without actually touching each other. There are spatial gaps between the atoms in a bat and a baseball, so ...
Landau Gauge Quark Propagator with External Magnetic Fields
Landau Gauge Quark Propagator with External Magnetic Fields

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History of quantum field theory

In particle physics, the history of quantum field theory starts with its creation by Paul Dirac, when he attempted to quantize the electromagnetic field in the late 1920s. Major advances in the theory were made in the 1950s, and led to the introduction of quantum electrodynamics (QED). QED was so successful and ""natural"" that efforts were made to use the same basic concepts for the other forces of nature. These efforts were successful in the application of gauge theory to the strong nuclear force and weak nuclear force, producing the modern standard model of particle physics. Efforts to describe gravity using the same techniques have, to date, failed. The study of quantum field theory is alive and flourishing, as are applications of this method to many physical problems. It remains one of the most vital areas of theoretical physics today, providing a common language to many branches of physics.
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