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101, 160401 (2008)
101, 160401 (2008)

... Introduction.—In recent years, the physics of the 2D chiral p-wave (px þ ipy ) superfluids has attracted much attention [1] because of its nontrivial statistical properties [2] and potential application in topological quantum computation [3,4]. The chiral superfluid can also act as a test bed for st ...
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... associated to a bosonic system can be obtained from the (hyper)contractivity of the semigroup e−tAγ : L2 (Rd , γ) → L2 (Rd , γ), where Aγ is the Dirichlet form operator for the Gaussian measure γ on Rd . After some contributions [12, 18, 36] Nelson finally proved in [32] that the previous semigroup ...
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... limitation of the sum in Eq. 共3兲 does not change the calculated van der Waals shifts by more than about 1%. By restricting the sum in the described way, we find that typically of the order of hundreds of two-particle states 兩n⬘ , ᐉ⬘ , j⬘ , m⬘j 典 丢 兩n⬙ , ᐉ⬙ , j⬙ , m⬙j 典 still contribute, although the ...
Module P11.1 Reflection and transmission at steps and barriers
Module P11.1 Reflection and transmission at steps and barriers

... side and there is a probability that the associated particle will tunnel through. A narrow region of high potential energy is called a potential barrier. Quantum mechanics therefore predicts two effects totally alien to the classical mechanics based on Newton’s laws: (i) particles may be reflected b ...
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“Anticoherent” Spin States via the Majorana Representation

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... 共200⫻ 30 Å2兲 self-assembled QDM’s. So far, most experiments on self-assembled QDM’s are optical3 and most theories are based on continuum models, such as effective mass approximations.3 These simple models ignore or drastically simplify important real material properties such as strain, atomistic sy ...
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¶ ÍÒ Ú Ö× Ø Ø¹ÍØÖ Ø, Report number:ITF-UU

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... their differential form. Vector analysis and differential equations are used throughout. Emphasis on solving boundary value problems, such as those appropriate to fields at interfaces between two media. Prerequisite: PHYS 203 and MATH 283; MATH 355 and MATH 380 strongly recommended. Offered in even ...
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... length as opposed to a positive scattering length given comparable magnitudes @26#. We note also that exceptions to this rule could occur if there are resonances in the relevant energy range. Although 39K in its spin-polarized u 22& state seems an unlikely candidate for BEC, the u 1,21 & state remai ...
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... to  N other su h states. With probability / N one of them will be in resonan e with the initial state, provided the on-site energies are uniformly distributed over a nite-width band. For large N this leads to state hybridization over time  J 1 , where J is the intersite hopping integral (we set ~ ...
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... no reliable method to describe even simple superconductors within post-HF methods, whereas within QMC it is now possible to describe by means of a simple correlated wave function both Mott insulators and high temperature superconductors, and more generally qualitative new effects that go beyond simp ...
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... uantum control pulses and NV centers appear as y level diagrams of the NV center electron spin agnetic field splits the NV spin triplet electronic d by the spin sublevels mS = 0 (labeled j0〉) and NV1. For the pulsed experiments, the same Rabi ...
Full Text - University of Arizona
Full Text - University of Arizona

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QUANTUM MECHANICS B PHY-413 Note Set No. 7

... components. This can be illustrated with Figure 1, which shows a vector of known length and projection onto the z-axis, but which can have any position on the circle obtained by rotating the vector around the b 2 , but not bz are also eigenfunctions of L z-axis. In formal terms our result tells us t ...
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HQ-1: Conference on the History of Quantum Physics Max Planck

... It would take almost two decades to confirm this equation experimentally. We see, in sum, that Einstein’s arguments for light quanta were based upon Boltzmann’s statistical interpretation of the entropy. He did not propose his light-quantum hypothesis “to explain the photoelectric effect,” as physic ...
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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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