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Band-gap structure and chiral discrete solitons in optical lattices with
Band-gap structure and chiral discrete solitons in optical lattices with

PH213 Chapter 27 Solutions
PH213 Chapter 27 Solutions

... Notice that this expression is valid for both positive and negative charges as well as for points located on the positive and negative z axis. If the charge is positive, the electric field should point outward. For points on the positive z axis, the field points in the positive z direction, which is ...
Measurements in Quantum Optics
Measurements in Quantum Optics

Quantum Information Chapter 10. Quantum Shannon Theory
Quantum Information Chapter 10. Quantum Shannon Theory

Electric Forces and Electric Fields
Electric Forces and Electric Fields

Three-Level L-Type Atomic System Localized by the Parameters of
Three-Level L-Type Atomic System Localized by the Parameters of

ATLAS and CMS
ATLAS and CMS

... discovered at yet higher-energy accelerators?  Are the quarks and leptons really fundamental, or do they, too, have substructure?  How can the gravitational interactions be included in the standard model? ...
Linear Collider - University of Victoria
Linear Collider - University of Victoria

... Collider overlapping that of the Large Hadron Collider. We therefore strongly recommend the expeditious construction of a Linear Collider as the next major international High Energy ...
Behavior of Charged Particles in a Biological Cell
Behavior of Charged Particles in a Biological Cell

On early and late phases of acceleration of the
On early and late phases of acceleration of the

About Mechanics of Virtual Reality
About Mechanics of Virtual Reality

CDM article on quantum chaos - Department of Mathematics
CDM article on quantum chaos - Department of Mathematics

Chapter 3: Quantum Computing
Chapter 3: Quantum Computing

... the bandwidth for transmission of classical information, still in certain cases entangled states can be compressed to fewer qubits. This quantum compression could have important applications in practice, where the number of usable qubits is very limited. Schumacher [101] considered compression and d ...
pptx - IHES
pptx - IHES

Geometries, Band Gaps, Dipole Moments, Ionization Energies and
Geometries, Band Gaps, Dipole Moments, Ionization Energies and

Quantum Information Processing: Algorithms, Technologies and
Quantum Information Processing: Algorithms, Technologies and

... for transmission of classical information, still in certain cases entangled states can be compressed to fewer qubits. This quantum compression could have important applications in practice, where the number of usable qubits is very limited. Schumacher [101] considered compression and decompression o ...
The Addition Theorem for Spherical Harmonics and Monopole
The Addition Theorem for Spherical Harmonics and Monopole

... The key point is to observe that the angular momentum operators in both cases satisfy the same SU(2) algebra. The only difference is that, for ordinary angular momentum operators L, they satisfy ^r:L = 0, where ^r is the radial unit vector. For the monopole angular momentum operators J, we have the ...
Two-Fluid Model for Heavy Electron Physics
Two-Fluid Model for Heavy Electron Physics

Delayed-choice gedanken experiments and their realizations
Delayed-choice gedanken experiments and their realizations

Synthesis and properties of single luminescent silicon quantum dots
Synthesis and properties of single luminescent silicon quantum dots

... The fabrication of silicon nanocrystals and the investigation of their optical properties on a single-dot level in order to reveal the basic mechanism of luminescence was the main goal of the present work. It is extremely difficult to control several nanometer size objects with ordinary macroscopic ...
Contradiction within Paraxial Wave Optics and its - LAS
Contradiction within Paraxial Wave Optics and its - LAS

... In this paper a solution is proposed within a particle picture of the optical resonator as presented recently by the author [2], which is slightly modified in the present paper. This particle picture shows that the transverse modes can be understood as the transverse quantum mechanical eigenfunction ...
Numerical Renormalization Group Calculations for Impurity
Numerical Renormalization Group Calculations for Impurity

... All the three impurity models studied show second order quantum phase transitions and quantum critical points but the levels of understanding of each case, particularly to the issues of quantum phase transitions, are quite different for historical reasons. The soft-gap Anderson model (Withoff and Fr ...
FrustrationVSFactorization - School of Mathematical Sciences
FrustrationVSFactorization - School of Mathematical Sciences

Schroedinger`s cat states generated by the environment
Schroedinger`s cat states generated by the environment

... photons [7, 8]. Alternatively, large spin characterizes macroscopic atomic ensembles that are entangled via interaction with a common light source [9]. The weakness of their interactions with the environment renders large-spin ensembles robust against decoherence and thus makes them good candidates ...
Spooky Action at Spacy Distances
Spooky Action at Spacy Distances

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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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