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1. QUARK MODEL
1. QUARK MODEL

... Mesons have baryon number B = 0. In the quark model, they are qq ′ bound states of quarks q and antiquarks q ′ (the flavors of q and q ′ may be different). If the orbital angular momentum of the qq ′ state is ℓ, then the parity P is (−1)ℓ+1 . The meson spin J is given by the usual relation |ℓ − s| ≤ ...
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... move the ‘center of gravity’ of the course from the microwave range to the optical one and supply the course with new sections. However, one should keep in mind that lasers and masers are based on common principles and that quantum electronics originated from radio spectroscopy and radiophysics. The ...
The use of spin-pure and non-orthogonal Hilbert spaces in Full
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Fluctuations of kinematic quantities in p+p interactions at the CERN

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Lecture Notes for Physics 229: Quantum Information and Computation

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... the Curie temperature the magnetic moments of the system align, giving rise to a non-zero magnetic moment and the ferromagnetic state emerges. In this ferromagnetic state, the rotational symmetry is broken. By considering the relation between the internal order and the symmetries of phases of matter ...
V. Linetsky, “The Path Integral Approach to Financial Modeling and
V. Linetsky, “The Path Integral Approach to Financial Modeling and

... on each path, and the exponential of the negative of this number gives a weight of the path in the path integral. According to Feynman, a path integral is defined as a limit of the sequence of finite-dimensional multiple integrals, in a much the same way as the Riemannian integral is defined as a li ...
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Non-Perturbative Aspects of Nonlinear Sigma Models

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... 4 Properties of Selected Higher-Dimensional Models ...
Analysis of General Geometric Scaling Perturbations in a Transmitting Waveguide: Fundamental Connection Between Polarization-Mode Dispersion and Group-Velocity Dispersion
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... is defined to be proportional to ␶.15 The desirable condition of zero PMD at a particular frequency ␻ then implies a zero value of the frequency derivative of the degeneracy split ⌬ ␤ e , or equivalently ⌬ ␤ e must be stationary at such a frequency. Finally, Eq. (7) permits perturbations that are, i ...
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Teaching Theoretical Physics: the cases of Enrico Fermi and Ettore

... kinetic energy, mean free path, equipartition of the energy, the phase space, the Boltzmann distribution law and the Maxwell velocity distribution. A second set dealt with electromagnetism: electromagnetic perturbation, the Poynting vector, the electronic theory of dispersion, radiation theory. Ferm ...
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... Objects tend to attempt to minimize their potential energy as much as possible. In Case C, the center of mass is lowest. Mechanics Lecture 18, Slide 4 ...
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... system: ZnCu3(OH)6Cl2, where a single electron spin resides on the Cu (10) (see the second figure, bottom panel). Although the exchange energy is ~200 K, this material does not show any magnetic ordering down to millikelvin temperatures. The magnetic excitations are apparently gapless, but unlike th ...
arXiv:math/0601458v1 [math.QA] 19 Jan 2006
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... in no ways on any other. The set of all Z-structures on S contains just S itself if S has exactly one element, and is empty otherwise. The cardinality of the type Z is easily seen to be just z. n Similarly, we have the type “being an n-element set”, denoted by Zn! , since it n has cardinality zn! . ...
Imaging Electrons in Few-Electron Quantum Dots
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Stationary two-atom entanglement induced by nonclassical two
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... eventually to the states |s and |a. 2.2. Nonidentical atoms The population distribution is quite different when the atoms are nonidentical with  = (ω2 − ω1 )/2 = 0. As before for the identical atoms, we use the master equation (1) and find four coupled differential equations for the density matr ...
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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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