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Classification of completely positive maps
Classification of completely positive maps

Many-Body Localization
Many-Body Localization

Charge dynamics and spin blockade in a hybrid double quantum dot
Charge dynamics and spin blockade in a hybrid double quantum dot

... In Fig. 2(a) we focus on a particular region of interest in the charge stability diagram, showing the classic signature of a double quantum dot through the presence of an extra ridge at the intersection between the charge transitions of a corner dot and the donor. The charge number (1,1) corresponds ...
Properties of electrons - VGTU Elektronikos fakultetas
Properties of electrons - VGTU Elektronikos fakultetas

... 1. Electrons are microparticles. 2. Quantum mechanics allows to reveal properties of microparticles. 3. Quantum theory, the branch of physics which is based on quantization, began in 1900 when Karl Ernst Ludwig Planck (1858 – 1947) published his theory explaining the emission spectrum of black bodie ...
Hamilton`s equations. Conservation laws. Reduction
Hamilton`s equations. Conservation laws. Reduction

Quantum fluctuations and thermodynamic processes in the presence of closed... by Tsunefumi Tanaka
Quantum fluctuations and thermodynamic processes in the presence of closed... by Tsunefumi Tanaka

... A closed timelike curve (CTC) is a closed loop in spacetime whose tangent vector is everywhere timelike. A spacetime which contains CTC’s will allow time travel. One of these spacetimes is Grant space. It can be constructed from Minkowski space by im­ posing periodic boundary conditions in spatial d ...
Understanding Electron Spin
Understanding Electron Spin



... in both QED and SED. We recall that these two theories have many features in common [11, 17, 18]. It is also interesting to recall that the classical effects of the zero-point radiation were discovered very early by M. Planck in the period 1911–1912. The quantum zero-point radiation was discovered l ...
Collective potential for large-N Hamiltonian matrix models and free Fisher information
Collective potential for large-N Hamiltonian matrix models and free Fisher information

... gluonic field (Aµ ) belongs to the adjoint representation of the structure group, is perhaps the most natural example of a field theory where the dynamical degrees of freedom are matrix valued. It is believed that the planar large N limit is the correct simplification to consider while trying to und ...
Fourier Transform, Period Finding and Factoring in BQP Lecture 4 1
Fourier Transform, Period Finding and Factoring in BQP Lecture 4 1

... Let us compute the chance of finding the correct period with t samples. Suppose after repeating t times, we have not found the desired period M/r, but instead a multiple, say λ M/r. This means that each of the t samples must be a multiple of λ M/r. There are M/(λ M/r) = r/λ multiples of λ M/r, and s ...
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Lecture I: Collective Excitations: From Particles to Fields Free Scalar
Lecture I: Collective Excitations: From Particles to Fields Free Scalar

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pdf

... correct   answer)   was   preferred   by   those   who   disagreed   (69%).     We   conclude   from   this   that,   among   students   of   introductory   classical   physics,   those   who   disagree   with   No.   41   primarily   concern ...
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Flow of zero-point energy and exploration of phase space in

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Liquid-State NMR Quantum Computing

... y axis” is in the state (|0" + i|1")/ 2, etc. A spin-1/2 particle is thus more than just an ordinary bit. Any two-level quantum system, such as a spin-1/2 particle, can serve as a quantum bit (qubit). The difference between the quantum and classical descriptions becomes clear as soon as more than on ...
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"Liquid-State NMR Quantum Computing" in

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QUANTUM ALGORITHMS FOR ELEMENT DISTINCTNESS∗ 1

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... Incompleteness, Non-Locality and Realism. In this book, Redhead describes three different views on quantum mechanics (A: hidden variables, B: propensities and potentialities, and C: complementarity) and, although he does not develop the second view in any detail, he seems to favour it over the alter ...
Ketterle lecture notes July 13th - Quantum Optics and Spectroscopy
Ketterle lecture notes July 13th - Quantum Optics and Spectroscopy

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On inelastic hydrogen atom collisions in stellar atmospheres
On inelastic hydrogen atom collisions in stellar atmospheres

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Statistical Mechanics Contents 1 Thermodynamics

Time Symmetry and the Many-Worlds Interpretation - Philsci
Time Symmetry and the Many-Worlds Interpretation - Philsci

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New Approaches in Deep Laser Cooling of Magnesium Atoms for

... laser cooling, it is used everywhere in a MOT (in 3D case, of course, one have three pairs of σ+ and σ– waves). In this section we neglect the influence of a static magnetic field on the kinetics of atoms assuming the field to be sufficiently small at the scale of a cloud in the trap. This influence ...
Quantum Hall effect
Quantum Hall effect

... tron edge states in graphene in the Quantum Hall effect regime can carry both c We show that spin splitting of the zeroth Landau level gives rise to counterpropagat pposite spin polarization. These chiral spin modes lead to a rich variety of spin curr ding on the spin flip rate. A method to control ...
EPR, reuscitate cat
EPR, reuscitate cat

... I have no idea how you would express “liveness” as a quantum operator, much less how you would find a measurable quantity, B, that is incompatible with it. Classical observables do not behave this way – incompatibility applies to the quantum realm only. Why? *shrugs* ...
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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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