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Anomaly driven signatures of new invisible physics
Anomaly driven signatures of new invisible physics

Helium atom - ChaosBook.org
Helium atom - ChaosBook.org

... determinants. We need to determine their phase space trajectories and calculate their periods, topological indices and stabilities. A restriction of the periodic orbit search to a suitable Poincaré surface of section, e.g. r2 = 0 or r1 = r2 , leaves us in general with a 2-dimensional search. Method ...
Quantum Field Theory: Underdetermination, Inconsistency, and
Quantum Field Theory: Underdetermination, Inconsistency, and

copyrighted material
copyrighted material

... the wave function of the system under consideration. In 1927 Max Born proposed his probabilistic interpretation of wave mechanics: he took the square moduli of the wave functions that are solutions to the Schrödinger equation and he interpreted them as probability densities. These two ostensibly dif ...
Author`s personal copy
Author`s personal copy

Helium atom - ChaosBook.org
Helium atom - ChaosBook.org

... quantum mechanical properties of nothing less than the helium, a dreaded threebody Coulomb problem. This sounds almost like one step too much at a time; we all know how rich and complicated the dynamics of the three-body problem is – can we really jump from three static disks directly to three charg ...
Is a random state entangled ?
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Emergence of a classical world from within quantum theory
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... The starting point of this dissertation is that a quantum state represents the observer’s knowledge about the system of interest. As it has been pointed out several times by the opponents of this epistemic interpretation, it is difficult to reconcile this point of view with our common notion of “phy ...
Path Integral Formulation of Quantum Tunneling: Numerical Approximation and Application to
Path Integral Formulation of Quantum Tunneling: Numerical Approximation and Application to

On the Exact Evaluation of Certain Instances of the Potts Partition
On the Exact Evaluation of Certain Instances of the Potts Partition

Entangling Dipole-Dipole Interactions and Quantum Logic in Optical
Entangling Dipole-Dipole Interactions and Quantum Logic in Optical

... quantum states can be prepared by cooling to the vibrational ground state of the optical lattice using Raman sideband cooling [18], or perhaps by loading the lattice with a precooled sample of Bose-condensed atoms [19]. Both internal and external degrees of freedom can be further manipulated through ...
Seeing a single photon without destroying it
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Quantum phenomena in gravitational field - AEgIS
Quantum phenomena in gravitational field - AEgIS

... 2. Quantum states of ultracold antihydrogen above material surface (Alexei Voronin) In the context of the general relativity theory, universality of a free fall is often referred to as the Weak Equivalence Principle (WEP). WEP is being tested with increasing sensitivity for macroscopic bodies. The b ...
Topological insulator with time
Topological insulator with time

Alignment and Survey - Oxford Particle Physics home
Alignment and Survey - Oxford Particle Physics home

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Spin and photophysics of carbon-antisite potential quantum bit Linköping University Post Print

... reconstruction. For instance, in the triplet ground state of hh complex we found a distance of 2.71 Å between the symmetrically equivalent Si atoms, marked as Si2 in Fig. 2, and distances of 3.03 Å between the Si atom, located on the mirror plain of C1h symmetry and marked as Si1 in Fig. 2, and th ...
Part II Applications of Quantum Mechanics Lent 2012
Part II Applications of Quantum Mechanics Lent 2012

Department of Physics, Chemistry and Biology Master’s Thesis Thomas Fransson
Department of Physics, Chemistry and Biology Master’s Thesis Thomas Fransson

... The Hartree–Fock (HF) approximation forms an approximate electronic wave function as a single Slater determinant. This construction of the wave function and the Hamiltonian from Eq. 2.4 gives a ground-state HF wave function as obtain by the variational principle EHF = minhΨ(λ)|Ĥ|Ψ(λ)i ≥ E0 , ...
Information theoretic treatment of tripartite systems and quantum
Information theoretic treatment of tripartite systems and quantum

... being present in a third system c. In Sec. V of this paper we present quantitative generalizations of this and some other “all-or-nothing” theorems to situations in which, for example, almost all information of the w type of information about a is in b and one wants to bound how much v information, ...
Ice, spin ice and spin liquids  lecture April 16, 2013
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... It would thus appear that we are done, having explained both significant facts about spin ice. However, this is not the case. First, the nearest-neighbor Ising antiferromagnet is not so simple after all; in fact, it exhibits a divergent correlation length as T ! 0, which cuts off algebraic, dipolar ...
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... The neutrino experimental facility at J-PARC was built to produce the world’s highest intensity neutrino beam and to facilitate leading research into neutrino physics. Its beam power is rated at 750 kW. In 2013, the facility was operated at 230 kW, which led to the first-ever definitive observation ...
Position and momentum in quantum mechanics
Position and momentum in quantum mechanics

Nonequilibrium Fermi Golden Rule for electronic transitions
Nonequilibrium Fermi Golden Rule for electronic transitions

Spin-orbit coupling effects in two
Spin-orbit coupling effects in two

Quantum Computation and Quantum Information
Quantum Computation and Quantum Information

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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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