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Measurement-based and Universal Blind Quantum Computation
Measurement-based and Universal Blind Quantum Computation

Quasi-exact treatment of the relativistic generalized
Quasi-exact treatment of the relativistic generalized

Exploring a Classical Model of the Helium Atom
Exploring a Classical Model of the Helium Atom

... region decreases. We have plotted the region where tori exist in Fig. 2 for CF-l (circular configuration). Here the initial velocity VI is varied by fixing the radius (Xl)' The lower limit of Xl is about 1.45. Though the tori have a finite measure in the phase space, the region of existence is not c ...
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Spin transport through nanostructures B. K ,

... without collective excitations. At zero magnetic field, the total-spin up and totalspin down components are energetically degenerate, and separated from the ground state n = 2q, s = 0,0,0 by δEp = 2p2Eσ. States with an odd number of electrons, n = 2q + 1, can be considered similarly. Here, the excit ...
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... The next step is to compute the average of the two rates (1.9) in the resemoir state. Such a calculation is not trivial. First, Rf(t) does not cornmute with Si(t) and G(t). Secondly, the system observables Si(t) and G(t) also operate on resemoir states since they have been « contaminated » by resemo ...
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... Wavefunctions for particle in the box • What does the energy look like? ...
Including Nuclear Degrees of Freedom in a Lattice Hamiltonian, P. L. Hagelstein, I. U. Chaudhary, This paper has been accepted for publication in J. Cond. Mat. Nucl. Sci. and will be published soon. An earlier version was posted on the LANL ArXiV (/0401667 [cond-mat.other] 20 Jan 2012).
Including Nuclear Degrees of Freedom in a Lattice Hamiltonian, P. L. Hagelstein, I. U. Chaudhary, This paper has been accepted for publication in J. Cond. Mat. Nucl. Sci. and will be published soon. An earlier version was posted on the LANL ArXiV (/0401667 [cond-mat.other] 20 Jan 2012).

... there were no physical transitions which could serve as the strongly coupled two-level transition within the model. We were optimistic in our writing about the possibility that systems described by three-level systems (or N-level systems) would be able to do the job. After putting in a great deal of ...
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... like a quantum gas, a gas where quantum mechanical effects are important. The quantum mechanical effect which we see on play here is the Pauli exclusion principle: Two fermions cannot occupy the same energy state. To understand this principle we need to dig even deeper into the quantum theory. Accor ...
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... IN measurement of excitation cross sections of energetic ions or atoms in collisions with gas molecules, we must consider the following fact. In the apparatus usually used for this type of experiment, a monoenergetic beam of the ions or atoms being studied enters a collision chamber filled with gas ...
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Spatial and Temporal Wave Functions of Photon
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... the adiabatic theorem. The second proof is self contained, and does not require knowledge of the adiabatic theorem. Instead it uses the simple Zeno effect[38], thus providing an alternative point of view of adiabatic algorithms using measurements (Such a path was taken also in [11].) This implies th ...
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Quantum Chromodynamical Explanation of the Strong Nuclear Force

... The Strong Nuclear Force was proposed to explain the unintuitive attraction between protons and neutrons within an atomic nucleus, despite the relatively immense repulsion of the electromagnetic force overshadowing the attraction between the particles due to gravitation. It is responsible for bindin ...
The Membrane Vacuum State
The Membrane Vacuum State

... back to the very depths of the sixties, thus predating the emergence of its more illustrious and celebrated sibling, string theory. The birthplace of membrane theory, like many other grand ideas, was in the brilliant mind of Dirac [1]. In 1962, Dirac was pursuing an alternative model for the electro ...
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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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