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hdwsmp2011 - FSU High Energy Physics
hdwsmp2011 - FSU High Energy Physics

... particles with material in the detector; detectors usually have some “amplification” mechanism to render result of this interaction observable  Many detection techniques have been developed over the last century  breakthrough in detection techniques often led to breakthrough discoveries  many of ...
The New Minimal Standard Model
The New Minimal Standard Model

... In this letter, we advocate a different and conservative approach to physics beyond the MSM. We include the minimal number of new degrees of freedom to accommodate convincing (e.g., > 5σ) evidence for physics beyond the MSM. We do not pay attention to aesthetic problems, such as fine-tuning, the hie ...
Monday, Apr. 11, 2005
Monday, Apr. 11, 2005

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8. Quantum field theory on the lattice
8. Quantum field theory on the lattice

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Dual approaches for defects condensation
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... The quantum field theory description of a physical system relies on a proper identification of its degrees of freedom which are then interpreted as excited states of the fields defining the theory. However it is sometimes the case that the theory may contain important structures which are not descri ...
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Supersymmetry

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Gregory Moore - Rutgers Physics
Gregory Moore - Rutgers Physics

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Electroweak precision data and right-handed gauge bosons

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Ten Lectures on the ElectroWeak Interactions
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Two Times - University of Southern California
Two Times - University of Southern California

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Non-Equilibrium Dynamics and Physics of the Terascale

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ppt - Desy

... • Probably it arises from an experimental problem • Then it is very unfortunate because [sin2q]l vs [sin2q]h makes the interpretation of precision tests ambigous Choose [sin2q]h: bad c2 (clashes with mW, …) Choose [sin2q]l: good c2, but mH clashes with direct limit ...
strings - BCTP, Bonn
strings - BCTP, Bonn

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Quantization of the Radiation Field
Quantization of the Radiation Field

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Massive two-loop Bhabha Scattering --- the - Indico

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Asymptotic Freedom and Quantum
Asymptotic Freedom and Quantum

... This fact cast some doubts on the validity of the original explanation of the Meissner effect within the BCS theory, which, though well motivated on physical grounds, was not gauge invariant. Nambu finally put these doubts to rest after earlier contributions by Philip Anderson (Nobel Prize, 1977) an ...
ibm_seminar - Stony Brook University
ibm_seminar - Stony Brook University

... But the 4 fermion interaction violates unitarity for energies above about 600 GeV. In analogy with W+ QED, postulate spin 1 boson carrier, W+. The W+ e n must be heavy to give the short range observed for the Weak Int’n, thus theory non-renormalizable. s-wave unitarity violations, ...
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... where z-component operators s1z and s2z are coupled to bath spins represented by σnkz . Here n = 1, 2 labels the baths and k = 1, 2, 3, ..., Nn labels the individual spins in the baths. For exchange symmetric case parameters of the two baths are taken to be identical. In conclusion, exchange symmetr ...
More on the MASS GAP and YANG-MILLS
More on the MASS GAP and YANG-MILLS

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All three experiments have identified specific B meson decays and
All three experiments have identified specific B meson decays and

... studies looked at decays of the B meson that involve leptons – electrically charged elementary particles and their associated neutrinos. There are three charged leptons: the electron, a critical component of atoms discovered in 1897; the muon, first observed in cosmic rays in 1937; and the much heav ...
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list_of_posterpresentation

... “Matrix model and random matrix theory analysis of protein” Abstract: Static and dynamical structures of protein is analyzed using the matrix model and the random matrix theory, respectively. Protein 3d structures registered in PDB [1] exceed 100,000 kinds and the detailed analysis becomes current ...
Introduction to the Standard Models of Particle Physics and Models
Introduction to the Standard Models of Particle Physics and Models

... what would the new particle have to be like? doesn’t interact with light (electromagnetism) or strong force about 80% of all matter ...
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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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