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Holographic Quantum Error Correcting Codes - Adrian Franco
Holographic Quantum Error Correcting Codes - Adrian Franco

Three-dimensional Child–Langmuir law for uniform hot electron
Three-dimensional Child–Langmuir law for uniform hot electron

... been a subject of much interest in recent years.8–13 For uniform cold electron emission, a 2D planar classical CL law has been derived analytically,8 which agrees well with the simulation results.9 Enhanced emission near to the beam edges has also been reported in various 2D nonuniform emission mode ...
PACS numbers: 32.80.Pj, 42.50.Vk, 89.80.+h In a quantum computer
PACS numbers: 32.80.Pj, 42.50.Vk, 89.80.+h In a quantum computer

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... Quantum States and Superposition: While classical bits exist in only one of the binary states at any given time, quantum bits, or qubits, can exist in a superposition state, which is a linear combination of the |0i and |1i states. This extends to multiple qubits, i.e. a quantum mechanical system wit ...
Optimization of quantum interferometric metrological sensors in the
Optimization of quantum interferometric metrological sensors in the

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PDF

... loading protocol is repeated—unless exactly one memory at each end has absorbed a photon. In the limit of large K, this scheme converts all multiphoton events into erasures. The only loading events that remain are those in which a single photon entered exactly one of the memories at each end of the ...
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PDF ∗ , 88K - UCLA Chemistry and Biochemistry
PDF ∗ , 88K - UCLA Chemistry and Biochemistry

... interference disappears and conductance resumes. This can be seen in Figure 4, where the mere raising of the potential energy of one of the CH sites in the cross-linker or the change in the coupling strength of one bond strongly affects the conductance of the molecular wire. How general are these re ...
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... According to the Josephson equations, the classical canonical momentum P = is proportional to the charge Q or to the number of Cooper pairs Q/2e on the capacitor according to P = ~Q/2e. The quantum Hamiltonian can then be written as HJJ = Ec N 2 + U, ...
Chapter 6 | Thermochemistry
Chapter 6 | Thermochemistry

... (a) The set of quantum numbers n = 2, = 0 describes a 2s orbital that can be occupied by two electrons. (b) The set of quantum numbers n = 3, = 1, m = 0 describes one of the 3p orbitals that can be occupied by two electrons. (c) The set of quantum numbers n = 4, = 2 describes the set of 4d orbitals. ...
The world according to quantum mechanics (or, the 18 errors of
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Here - Blogs at UMass Amherst

... freedom and confinement. The weak interaction needed the Brout–Englert–Higgs mechanism, and also dimensional regularization for ’t Hooft’s proof of renormalizability. We only could formulate the Standard Model as a theory after all these QFT developments occurred. In contrast, General Relativity was ...
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... Most of the time this doesn’t matter, because the grid points are packed so densely that they might as well be a continuum. Particles can’t really be anywhere, but they can be nearly anywhere. However, there are some situations where it does matter. In the classical picture, the probability of being ...
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Ionization of high-lying states of the sodium atom by a pulsed
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Three Myths about Time Reversal in Quantum Theory
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... Potential: U(x) = -Wd2(x2+d2)/(x4+8d4) Sketch this potential & discuss motion at various x. Is it bounded or unbounded? Where are the equilibrium positions? Are these stable or unstable? Find the turning points for E = -W/8. ...
University of Maryland, Baltimore County
University of Maryland, Baltimore County

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... Consider a collection of bombs so sensitive that a collision with any single particle (photon, electron, etc.) Bomb absent: is guarranteed to trigger it. Only detector C fires BS2 that certain of Suppose the bombs are defective, but differ in their behaviour in no way other than that Bomb present: t ...
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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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