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Hadron Collider Summer School
Hadron Collider Summer School

... The TEVATRON is presently the ‘energy frontier’ collider in operation at FNAL, with a beam energy of 980 GeV and a size of ~ ¼ LHC. It is the first super-conducting collider ever build. It collides proton and anti-proton bunches that circulate in opposite directions in the SAME vacuum chamber. The T ...
Spin Conductivity in Two-Dimensional Non
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... We notice that the lowest and highest values of the excitation spectrum in magnetic Brillouin zone determine the threshold of low- and high-frequency limits of the spin conductivity. We also note that the lower bound of the spin conductivity spectrum at low fields h/J ≤ 1 is determined by the excita ...
Editorial Inaugural Issue Let All Truth Seekers Be the Vessels to
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... “sentience is covertly connected to space-time geometry when axioms of congruency are stipulated, essentially hiding in the formality what is sense-certain.” The work of Dick Richardson illustrates from the mystical point of view “consciousness, time and prespacetime as consciousness finds it to be. ...
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... we focus on understanding the lattice thermal transport properties of carbon nanotubes. The method employed here [8] is general and can be applied to many other systems. Due to the technological difficulties of synthesizing high-quality and well-ordered nanotubes, it is still challenging to perform ...
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... Even those who claim to hold to philosophies other than materialism are influenced by it, perhaps in ways they are completely unaware of. Its fundamental principle is that matter and energy are primary and all else is secondary, in the sense that all else is derived from, or is an outgrowth of, matt ...
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... in quantum dots. As a further application of this theory, we use it to demonstrate the feasibility of measuring the phonon spectra and distribution functions, by exploiting the driving-field dependence of the effective damping rates. We propose and analyze two forms of such spectroscopy, one based o ...
Electronic Structure of Clusters and Nanocrystals
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... There is one notable difference in the Hartree-Fock summations compared to the Hartree summation. The Hartree-Fock sums include the i = j terms in Eq. §.13. This difference arises because the exchange term corresponding to i = j cancels an equivalent term in the Coulomb summation. The i = j term in ...
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... is the Berry phase. The last term in the latter equation arises when the states |n(R)i are not a single-valued function of R in the region of interest of the parameter space2 , and is given by αn (C) = i ln [hn(R(0))|n(R(T ))i] . ...
Monogamy and ground-state entanglement in highly
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Nonlinear Quantum Optics in a Waveguide: Distinct Single Photons Strongly
Nonlinear Quantum Optics in a Waveguide: Distinct Single Photons Strongly

... is allowed, which can result in the transmission of photon a through the reflective barrier. The distinguishing feature of waveguide QED is the strong resonant interference of scattered and incident photons by the atomic transition of a single atom [15]. Strong coupling between the atom and the wave ...
Multi-species systems in optical lattices: effects of disorder
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... interacting system at zero temperature for both symmetric and asymmetric lattices. This material is the content of Paper I. We continue with the strongly correlated regime in Chapter 5, where we investigate the Mott insulator phase of various systems in the p and d bands in terms of effective spin m ...
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... asymptotes to RC for M  MPl and RS for M  MPl . Models in which this function is symmetric under the duality transformation M ↔ 1/M (such as the linear and quadratic forms given above) are said to satisfy the strong BHUP correspondence [20]. One controversial implication of the BHUP correspondence ...
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... first the kinetic energy in the Schrödinger has the usual form described by the d-dimensional Laplacian and that the electrostatic interaction in the Schrödinger equation has the same form irrespective of the spatial dimension. This of course leads to modified Maxwell equations in higher dimension ...
Phase Transitions - Helmut Katzgraber
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... This implies that for the limit N → ∞ the energy difference goes to minus infinity which means that the building of a domain wall is energetically more favourable. More and more domain walls are built and we will not observe a state with all spins up (or down). Thus there is on phase transition in o ...
CHAPTER 14: Elementary Particles
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... entanglement and relevant techniques such as majorization, are introduced. To illustrate some of the concepts reviewed here I discuss the entanglement properties of an exactly soluble many-body model which was studied in paper (E) of the publication list corresponding to the present Thesis. An alte ...
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... causal relevance relations even if the method of difference to establish the causal relevance relation was not applied to the entity itself. Instead, using well-known entities, you can establish causal relevance relations that are sufficiently general to be instantiated by the hitherto unknown entit ...
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... including 1/N corrections, scale invariance can be maintained only for one3 λ = λ0 . This would be acceptable, since m = 0, λ = λ0 would be natural due to scale invariance at that point. Our model has only two free parameters at large-N, ensuring predictive power. Here we address issues relevant to ...
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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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