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Possible large-N fixed-points and naturalness for O(N) scalar fields
Possible large-N fixed-points and naturalness for O(N) scalar fields

... A possibility is to build a model around a non-trivial UV fixed point. But existing work (conventional -, loop and perturbative expansions, numerics in the m–λ plane) does not indicate the presence of one2 . To find one in d = 4, it helps to have an expansion parameter. We look for a scale-invarian ...
Neutrino Oscillations
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... excluded from theories as they come from a class of interactions that lead to unacceptably rapid proton decay if they are all included. These models have little predictive power and are not able to provide a cold dark matter candidate. 1. More formally, the neutrinos are emitted in an entangled stat ...
The Physics of Inflation
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... underlying physics of this era. Over the next decade, the inflationary era – perhaps 10−30 seconds after the Big Bang – will thus join nucleosynthesis (3 minutes) and recombination (380,000 years) as observational windows into the primordial universe. However, while the workings of recombination and ...
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... the discovery of a stable phase with deconfined spinons in a model of quantum dimers on the 共geometrically frustrated兲 triangular lattice, i.e., a spin liquid.1 Beyond the interest in fundamental theoretical issues of these models,1–3 physical realizations of these systems may have technological app ...
JPD@Muon potential
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... to extend lepton high energy frontier in the multi-TeV range with reasonable dimension, cost and power consumption Muon based Higgs factory takes advantage of a strong coupling to Higgs mechanism by s resonance ...
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... numbers of π, ρ, A1 , and σ-mesons. The Lagrange density coincides with that of the standard chirally invariant σ-model which is known to account quite well for the lowenergy aspects of meson physics. Here mesonization renders additional connection between quark and meson properties. It also makes t ...
Quantum interference in the field ionization of Rydberg atoms
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... has provided insight into the connection between a field and photon picture of the electron’s pathway to freedom [7]. In the case where the microwave frequency is close to that of the classical Kepler frequency a variety of interesting behaviors have been observed including resonances in the ionizat ...
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... in complex angular momentum plane. Would like to understand diffraction in terms of quarks, gluons and QCD (need a hard process) A worthwhile task: •Diffraction is a significant part of stot •Elastic cross section drives stot via optical theorem: dsel/dt|t=0 (stot)2 •Understanding diffraction in te ...
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... quarks of s= ½ in same state?) This is forbidden by Fermi statistics (Pauli principle)! Solution: there is a new internal degree of freedom (colour) which differentiate the quarks: Δ++=urugub •  This means that apart of space and spin degrees of freedom, quarks have yet another attribute •  In 1964- ...
universo feature
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... around this conguration are given in terms of an emergent U(1) gauge theory with a Chern-Simons topological term. We also address the stability of the three lowest lying states, showing a common critical temperature. We consider experimentally measurable signatures of the mean eld states, which c ...
pdf book - Lowndes County Historical Society Museum
pdf book - Lowndes County Historical Society Museum

... eternity), permanently fixed in potentiality, and God brings them out to actuality incessantly and perpetually ... He goes on transforming the possibilities (isti dadat, lit. 'preparednesses') that have been there from the beginningless past and that are (tehrefore) essentially uncreated, into infin ...
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... Radioactivity was observed before the discovery of the electron. We are still trying to uncover the nature of the weak force. It may be instructive to recall that it took about 30 years before scientists figured out what Beta decay was all about: ...
Introduction to Integrable Models
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... more powerful algebraic Bethe ansatz after we have finished with the simple case at hand. Here, we will rederive the XXX1/2 case by algebraic means and then generalize it to general spin s. I will also briefly sketch further generalizations, such as spin chains with higher rank symmetry algebra. Tow ...
Review on Nucleon Spin Structure
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... scattering (DIS) measured quark spin invalidates the constituent quark model (CQM). I will show that this is not true. After introducing minimum relativistic modification, as usual as in other cases where the relativistic effects are introduced to the non-relativistic models, the DIS measured quark ...
Dark Matter Candidates - SLAC
Dark Matter Candidates - SLAC

... long as the particles are relativistic. The well known example of neutrinos freeze out with g ≈ 10.75, prior to the freeze-out of electrons and positrons (which lowers g ). Thus the (massless) neutrino temperature is lower than the photon temperature in the present universe. The relic density of a ...
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... lowest possible field energy is zero. Note, however, that this configuration requires φ to be non-vanishing: φ = ±λ. It therefore follows that the vacuum for a system containing a Higgs-type field is not empty; it contains, in fact, a constant scalar field φvac ≡ hφi = ±λ. In quantum physics, the qu ...
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Higgs mechanism

In the Standard Model of particle physics, the Higgs mechanism is essential to explain the generation mechanism of the property ""mass"" for gauge bosons. Without the Higgs mechanism, or some other effect like it, all bosons (a type of fundamental particle) would be massless, but measurements show that the W+, W−, and Z bosons actually have relatively large masses of around 80 GeV/c2. The Higgs field resolves this conundrum. The simplest description of the mechanism adds a quantum field (the Higgs field) that permeates all space, to the Standard Model. Below some extremely high temperature, the field causes spontaneous symmetry breaking during interactions. The breaking of symmetry triggers the Higgs mechanism, causing the bosons it interacts with to have mass. In the Standard Model, the phrase ""Higgs mechanism"" refers specifically to the generation of masses for the W±, and Z weak gauge bosons through electroweak symmetry breaking. The Large Hadron Collider at CERN announced results consistent with the Higgs particle on March 14, 2013, making it extremely likely that the field, or one like it, exists, and explaining how the Higgs mechanism takes place in nature.The mechanism was proposed in 1962 by Philip Warren Anderson, following work in the late 1950s on symmetry breaking in superconductivity and a 1960 paper by Yoichiro Nambu that discussed its application within particle physics. A theory able to finally explain mass generation without ""breaking"" gauge theory was published almost simultaneously by three independent groups in 1964: by Robert Brout and François Englert; by Peter Higgs; and by Gerald Guralnik, C. R. Hagen, and Tom Kibble. The Higgs mechanism is therefore also called the Brout–Englert–Higgs mechanism or Englert–Brout–Higgs–Guralnik–Hagen–Kibble mechanism, Anderson–Higgs mechanism, Anderson–Higgs-Kibble mechanism, Higgs–Kibble mechanism by Abdus Salam and ABEGHHK'tH mechanism [for Anderson, Brout, Englert, Guralnik, Hagen, Higgs, Kibble and 't Hooft] by Peter Higgs.On October 8, 2013, following the discovery at CERN's Large Hadron Collider of a new particle that appeared to be the long-sought Higgs boson predicted by the theory, it was announced that Peter Higgs and François Englert had been awarded the 2013 Nobel Prize in Physics (Englert's co-author Robert Brout had died in 2011 and the Nobel Prize is not usually awarded posthumously).
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