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Unparticle_Dark_Matter_(GUT07)
Unparticle_Dark_Matter_(GUT07)

... • Beyond the SM (for model buildings in this LHC era): Are there totally unexpected phenomena which has not yet discovered so far? What would be expected to happen at LHC that might be originated from some unknown models, not only SUSY or extra dimensional models, etc.? This is basically the motivat ...
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... to understand why all states are equally populated from the perspective of dynamics. The Ergodic theorem is built on the symmetry of time-reversal, i.e., the rate at which one changes from state i to state j is the same as the rate at which one changes from state j to state i. Here, we can consider ...
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... amplitudes to higher energy, and study possible new resonances. This includes a curious one that can be generated by the hh-WW channel coupling alone, even if the perturbative elastic interaction vanishes. ...
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No Slide Title - Webcast

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Chapter 3 Basic quantum statistical mechanics of spin

... representation of an algebra A over C. Then let φ : V → V be a homorphism, i.e. φ(av) = aφ(v) for any a ∈ A and v ∈ V . Then φ = λI, where I is the identity matrix. A vector space V “over C” means that multiplying a vector by a complex number gives another vector in V . It turns out that in the spin ...
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Violation of Bell`s inequalities in a quantum realistic framework
Violation of Bell`s inequalities in a quantum realistic framework

... can be predicted with certainty and obtained repeatedly within such a context will be called a modality. Given these definitions, let us bind them together by the following rule: In QM, modalities are attributed jointly to the system and the context. This principle will be called “CSM”, referring to ...
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... group of rotation paths, and quantum physics. In 1927 Wolfgang Pauli formulated the theory of so-called spin 1/2 particles in R3 . Paul Dirac, in 1928, extended the theory to relativistic space-time. In classical mechanics, a rotating object possess an angular momentum vector. If one imagines ones s ...
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Bose-Einstein condensates with balanced gain and loss

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... will vary depending upon whether the experiment measuring that event was detailed (e.g., also assessed which slit the particle traversed en route to the screen) or less detailed (only assessed the particle's position on the detector screen). This paper will show that probability amplitude mechanics ...
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Identical particles

Identical particles, also called indistinguishable or indiscernible particles, are particles that cannot be distinguished from one another, even in principle. Species of identical particles include, but are not limited to elementary particles such as electrons, composite subatomic particles such as atomic nuclei, as well as atoms and molecules. Quasiparticles also behave in this way. Although all known indistinguishable particles are ""tiny"", there is no exhaustive list of all possible sorts of particles nor a clear-cut limit of applicability; see particle statistics #Quantum statistics for detailed explication.There are two main categories of identical particles: bosons, which can share quantum states, and fermions, which do not share quantum states due to the Pauli exclusion principle. Examples of bosons are photons, gluons, phonons, helium-4 nuclei and all mesons. Examples of fermions are electrons, neutrinos, quarks, protons, neutrons, and helium-3 nuclei.The fact that particles can be identical has important consequences in statistical mechanics. Calculations in statistical mechanics rely on probabilistic arguments, which are sensitive to whether or not the objects being studied are identical. As a result, identical particles exhibit markedly different statistical behavior from distinguishable particles. For example, the indistinguishability of particles has been proposed as a solution to Gibbs' mixing paradox.
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