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Quantum statistics: Is there an effective fermion repulsion or boson
Quantum statistics: Is there an effective fermion repulsion or boson

FrustrationVSFactorization - School of Mathematical Sciences
FrustrationVSFactorization - School of Mathematical Sciences

... "Hamiltonian & Gaps", 7/9/2010 ...
Meson spectroscopy - KVI - Center for Advanced Radiation
Meson spectroscopy - KVI - Center for Advanced Radiation

... • There are two transverse polarization states of the string, clockwise (+) or anticlockwise (-) about the quark-antiquark axis. • We define an angular component momentum about the axis (Λ) – The dependence of the string wave function on the angle γ about the axis is eiγΛ ...
Fractional topological insulators
Fractional topological insulators

... Two quantum numbers characterizing a fractional state: n– the (spin) Hall conductivity e* - the smallest charge allowed for an excitation The question – can the edge states be gapped out without breaking time reversal symmetry ? The answer is determined by the parity of n/e*: ...
Ultrafast geometric control of a single qubit using chirped pulses
Ultrafast geometric control of a single qubit using chirped pulses

... [8, 9]. The ingenious idea of using the geometric phase [10–12] to manipulate the qubit state was recently developed in a new direction called geometric quantum computing [13–16]. The adiabatic manipulation of a quantum system using only geometric phase has some advantages since it reduces the requi ...
Observation of even denominator fractional quantum Hall effect in
Observation of even denominator fractional quantum Hall effect in

ppt
ppt

... BGS represents the predictions of Swanson et al quark model. It is difficult to change quark model, as it can reproduce precisely the masses of almost all the known charmonium states (Swanson, hepph/0601110). For 2P states, earlier (quenched) lattice QCD predictions (CP-PACS and Chen) of their masse ...
The hydrogen atom as an entangled electron–proton system
The hydrogen atom as an entangled electron–proton system

... depends on the positions of the other particles, rather than on some average density. Consequently, in a system of interacting particles, the probability of finding two particles with given positions or momenta is not simply the product of the single-particle probabilities: We say that the particles ...
In situ via incoherent fluorescence George C. Cardoso, Prabhakar Pradhan,
In situ via incoherent fluorescence George C. Cardoso, Prabhakar Pradhan,

... When the rf intensity is increased a component of the BSO at 4␻ begins to develop, as predicted. For the data in Fig. 4, the second harmonic of the driving field is used to trigger a 100-MHz digital oscilloscope and the fluorescence signal is averaged 256 times. When the probe beam is tuned to the F ...
classification of phenomena of parapsychology from the point of
classification of phenomena of parapsychology from the point of

... • Wolf Messing could acquire information about a person by his or her handwriting. In the abovementioned book he wrote (Messing, 1990), “I have taken a sheet of paper with a text... I see that the hand which wrote the text is dead.” (It was established later that Messing’s ‘diagnosis’ was correct). ...
What General Chemistry Students Know (and Don`t Know) About
What General Chemistry Students Know (and Don`t Know) About

... Student6: Confused by amplitude. P: What are photons? S: They're particles with light. And transfer momentum like a particle. P: Could you perhaps draw for me what you mean by a wave-like motion? S: Yeah. A classic sine wave. P: And this represents the light wave? S: Mm-hmm. P: What's on the y-axis ...
What General Chemistry Students Know
What General Chemistry Students Know

... Student6: Confused by amplitude. P: What are photons? S: They're particles with light. And transfer momentum like a particle. P: Could you perhaps draw for me what you mean by a wave-like motion? S: Yeah. A classic sine wave. P: And this represents the light wave? S: Mm-hmm. P: What's on the y-axis ...
Efficient simulation of quantum state reduction
Efficient simulation of quantum state reduction

... The energy-based stochastic extension of the Schrödinger equation is a rather special nonlinear stochastic differential equation on Hilbert space, involving a single free parameter, that has been shown to be very useful for modeling the phenomenon of quantum state reduction. Here we construct a gen ...
of a quantum system or state - Hal-SHS
of a quantum system or state - Hal-SHS

An Order-Theoretic Quantification of Contextuality
An Order-Theoretic Quantification of Contextuality

... interpretations, both with and without agents. The second notable feature of this model is that it lends itself to a description that encompasses both classical and quantum systems under a single structure. Thus, ρ can represent the state of a classical, quantum, or hybrid system, as long as it is m ...
Danish-Sino Workshop on Strongly Interacting Cold Atomic Gases
Danish-Sino Workshop on Strongly Interacting Cold Atomic Gases

The Fermi-Hubbard model 11 The Hubbard model
The Fermi-Hubbard model 11 The Hubbard model

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

... 3D etc. When we consider an ensemble of N atoms, the states of such an ideal gas can be written in the Fock representation as |n~0 , n~1 , . . .i, where nm ~ denote the occupation numbers of the corresponding m-th ...
Chapter 6 The Quantum Wave Function Let`s just get to the point
Chapter 6 The Quantum Wave Function Let`s just get to the point

AQA A Physics - Particle Physics
AQA A Physics - Particle Physics

... observed particles and interactions involved no charge, single or multiple electron charges or their positive equivalent and these charge units were conserved in reactions. However, with β— decay, it was found that some mass-energy was missing. Specifically, when carbon-14 undergoes β— decay to nit ...
Vacuum Polarization and the Electric Charge of the Positron
Vacuum Polarization and the Electric Charge of the Positron

quantum dynamics of integrable spin chains
quantum dynamics of integrable spin chains

Ultralow threshold laser using a single quantum dot and a
Ultralow threshold laser using a single quantum dot and a

... To determine whether our device is capable of exhibiting laser action, we cannot use the conventional, macroscopic definition of threshold, that the gain of the optical mode equals the cavity losses. Instead, we follow the alternative definition given by Björk, Karlsson, and Yamamoto, that the mean ...
Majorana Fermions - Physics | Oregon State University
Majorana Fermions - Physics | Oregon State University

... the capacity to protect quantum information from decoherence. Whereas their featureless ground states have precluded their straightforward experimental identification, excited states are more revealing and particularly interesting owing to the emergence of fundamentally new excitations such as Major ...
CHEM-UA 127: Advanced General Chemistry I
CHEM-UA 127: Advanced General Chemistry I

... If we could neglect the electron-nuclear interaction, then the wave function would be a simple product Ψ(x, R) = ψelec (x)ψnucl (R). However, we cannot neglect this term, but it might still be possible to write the wave function as a product. We note, first, that most nuclei are 3-4 orders of magnit ...
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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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