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Chapter Thirteen Charged Particle Collisions, Energy Loss, Scattering
Chapter Thirteen Charged Particle Collisions, Energy Loss, Scattering

... The last step is achieved by, first, taking the time derivative; second, integrating over t to obtain a delta-function δ(ω + ω 0 ); and, finally, integrating over ω 0 . Because the electric field is real, E(−ω) = E∗ (ω). Similarly, x(−ω) = x∗ (ω); ...
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... Pauli Exclusion Principle: In 1926, Wolfgang Pauli discovered that a set of quantum numbers is specific to a certain electron. That is, no two electrons can have the same values for n, l, ml, and ms. Although the first three quantum numbers identify a specific orbital and may have the same values, t ...
Holonomic Quantum Computation with Josephson Networks
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... more detailed investigation of geometric phase effects in such systems. Here we show that non-Abelian phases can appear in the quantum dynamics of Josephson networks. As it will become clear in the following non-Abelian phases can be detected by a measurement of the adiabatic charge dynamics of the ...
High-order impulse approximation for calculating pulsed-field recombination F. Robicheaux
High-order impulse approximation for calculating pulsed-field recombination F. Robicheaux

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... iterative but the immediate zeroing gives us recursivity as well. A single fermion can only be ‘created’ if we simultaneously create the rest of the universe as a kind of reverse image, whose structure is completely defined. We don’t have to know how to construct the universe, only that it must have ...
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... often describable by master equations, Fokker-Planck equations, stochastic processes, etc. ...
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... (A, B ∈ E (H) ). First, when P and Q are orthogonal projections, then P ◦ Q = P QP is the accepted form for an ideal measurement in that case [2, 3, 4]. Second, ◦ satisfies various algebraic, continuity and duality conditions that one would expect from a sequential product. For example, for all A, B ...
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... technical considerations. One interesting feature of our design is that the IFM probe qubit acts only as an ancillary qubit, which is disentangled from the logical qubits at the end of the gate operation, so that no measurement of this qubit is required. The elimination of this measurement greatly b ...
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... Gaussian probability with standard deviation Dx. The Heisenberg uncerimportant benchmarks for the qual- tainty relation states that when simultaneously measuring incompatible proportional to 1/ N . This is a ity of a measurement, and they observables such as position x and momentum p, the product of ...
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... theory which is not both ad hoc and incompatible with special relativity, these assertions may seem plausible (cf. Deutsch 1996). It is certainly the case that, at least over short time intervals, quantum states can be found which will give apparently accurate representations of the physical states ...
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... appropriate background theory for all these logics is set theory: ‘ a  A ’ expresses that the element ‘a’ belongs to the set of individuals represented by ‘A’. In short, it is a universal and basic characteristic of traditional logic, and traditional thought in general, that there are individuals t ...
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Algorithmic complexity of quantum states
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... Classical algorithmic complexity [3] was first introduced to give an answer to the question: “is the classical string ω N = ωi1 ωi2 ωiN random?”. The definition is based on the concept of algorithmic reproducibility of a sequence: The algorithmic complexity KCl of a string ω N is the length of the s ...
Quantum Mechanics: Postulates
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... In order for Ψ(x, t) to represent a viable physical state, certain conditions are required: 1. The wavefunction must be a single-valued function of the spatial coordinates. (single probability for being in a given spatial interval) 2. The first derivative of the wavefunction must be continuous so th ...
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... different momentum, the more waves we need, the more possible values there are for a momentum measurement, which is trying to determine the wavelength. Conversely, the more accurate the wavelength or momentum, the less certain the position. A similar relation links observation time to the error in m ...
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Bohr–Einstein debates



The Bohr–Einstein debates were a series of public disputes about quantum mechanics between Albert Einstein and Niels Bohr. Their debates are remembered because of their importance to the philosophy of science. An account of the debates was written by Bohr in an article titled ""Discussions with Einsteinon Epistemological Problems in Atomic Physics"". Despite their differences of opinion regarding quantum mechanics, Bohr and Einstein had a mutual admiration that was to last the rest of their lives.The debates represent one of the highest points of scientific research in the first half of the twentieth century because it called attention to an element of quantum theory, quantum non-locality, which is absolutely central to our modern understanding of the physical world. The consensus view of professional physicists has been that Bohr proved victorious, and definitively established the fundamental probabilistic character of quantum measurement.
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