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Quantum Computation - School of Computing Science
Quantum Computation - School of Computing Science

One-Shot Classical Data Compression with Quantum Side
One-Shot Classical Data Compression with Quantum Side

PHYSICS III: Modern Essentials
PHYSICS III: Modern Essentials

Chapt. 5: Quantum Theory of the Hydrogen Atom
Chapt. 5: Quantum Theory of the Hydrogen Atom

... With some rearranging, the Balmer equation looks like this: ν = 3.29 x 1015 s-1 (1/22 - 1/n2) -This is the equation we just derived, but with nf fixed at a value of 2 -So, the Bohr model also accurately predicts the frequencies of the Balmer Series emission lines -BUT, it also predicts other emissio ...
Many-Body effects in Semiconductor Nanostructures Stockholm University Licentiat Thesis
Many-Body effects in Semiconductor Nanostructures Stockholm University Licentiat Thesis

... band, control of the materials conductivity may be achieved. This is often done by doping the semiconductor, placing impurities into the bulk and thereby injecting conductive electrons or holes into the band structure. The conducting particles in a semiconductor material, such as electrons in the co ...
Class 39 1
Class 39 1

... No two electrons can be in the same quantum state. In other words, no two electrons can possess the same set of four quantum numbers. The consequence of the Pauli Exclusion Principle is that when we fill the energy levels of an atom with electrons (where there are Z of them), we can only fill one el ...
Indistinguishable particles in quantum mechanics
Indistinguishable particles in quantum mechanics

... was then improved during the following decade, mainly by Arnold Sommerfeld and Alfred Landé, rendering it more sophisticated, trying to make it able to account for the multiplet structure of spectral lines, including for atoms in electric and magnetic fields. In 1922, Pauli joins the effort (actually ...
One-dimensional electron transport in
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Another Look at the Wigner Function
Another Look at the Wigner Function

Open Access - Scientific Research Publishing
Open Access - Scientific Research Publishing

Chapter 3 The Statistical Theory of Thermodynamics 3.1 Macrostate
Chapter 3 The Statistical Theory of Thermodynamics 3.1 Macrostate

... σ = ±1/2 is its spin quantum number. Notice that quantum states are discrete [i.e., the parameters (n, l, m, σ) are discrete numbers], contrast to the classical states, where the state parameters (r; p) are continuous variables. For a quantum particle moving in a box, its state is a plane-wave speci ...
Details of Approved Courses For Mphil/Ms, Mphil Leading To Phd
Details of Approved Courses For Mphil/Ms, Mphil Leading To Phd

Quantum field theory in curved spacetime
Quantum field theory in curved spacetime

... dependent on the state of motion of the detector, which is the so-called “Unruh effect”. This motivates us to study the notion of the vacuum in more detail, which leads to the conclusion that the ground state as defined in Minkowski coordinates |0M i need not be the same as in arbitrary coordinates. ...
Problems in Quantum Mechanics
Problems in Quantum Mechanics

The flashes of insight never came for free
The flashes of insight never came for free

Interaction-induced Lipkin-Meshkov-Glick model in a Bose
Interaction-induced Lipkin-Meshkov-Glick model in a Bose

... Received 27 Aug 2009; accepted 26 Sep 2009; published 15 Oct 2009 ...
PEPS, matrix product operators and the Bethe ansatz
PEPS, matrix product operators and the Bethe ansatz

... • Ground states have extremal local correlations: all (quasi-)long range correlations are a consequence of the fact that those local correlations must be made compatible with translational invariance ...
Quantum phase transitions in Kitaev spin models
Quantum phase transitions in Kitaev spin models

... show that the Kitaev spin model on the honeycomb lattice exhibits a continuous quantum phase transition. We also reveal the relationship between bipartite entanglement and the ground-state energy. Our approach directly shows that both the entanglement and the ground-state energy can be used to chara ...
Neutron Scattering Theory - Oklahoma State University
Neutron Scattering Theory - Oklahoma State University

... So, solving the Schrodinger equation in first-order Born approximation, the differential cross-section is given by above equation for a spherically symmetric potential. The potential is weak enough that the scattered wave is only slightly different from incident plane wave. ...


... the length of a body contracts in the direction of its motion continued to be president of Solvay Conferences until his when it is moving. This phenomenon is now called Lorentz death. contraction. Lorentz is also well-known for Lorentz Owen Williams Richardson (1879-1959) described transformations w ...
Grof, Jung, and the Quantum Vacuum
Grof, Jung, and the Quantum Vacuum

Foundations of Physics An International Journal Devoted to the
Foundations of Physics An International Journal Devoted to the

The Standard Model - University of Rochester
The Standard Model - University of Rochester

... Gluons act on something called color charge, which only quarks and gluons have ...
Violation of the Schiff theorem for unstable atomic - Plasma-Gate
Violation of the Schiff theorem for unstable atomic - Plasma-Gate

... (5) we see that expression (23) identically coincides with the energy shift (5) which is derived from the balance of momenta. In conclusion we formulate the results of the present work. The Schiff theorem (screening of an external static homogeneous electric field on the nucleus of a neutral atom) i ...
Powerpoint 6/22
Powerpoint 6/22

... The system. This is like calling the probability distribution the State of the system and confuses our description of the system with the physical state of the system. For our classical machine, the system is always in one of the states. For the quantum system, this type of statement is much trickie ...
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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.
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