32,181 research outputs found

    NEW PARTICLES AND INTERACTIONS

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    We analyze the manifestations of new matter particles predicted by models of new physics beyond the Standard Model, at present and future high--energy colliders. We consider both the production of these new particles and some of their indirect signatures at pppp and ePeP colliders as well as TeV \ee colliders with their \ee, e \gamma, \gamma \gamma and e−e−e^- e^- modes. The report is arranged into four main sections plus an overview. These sections will deal separately with exotic and excited fermions, difermions, and new interactions.Comment: 64 pages, latex, 30 figures (not included). The full *.ps file including the figures can be obtained via anonymous ftp at ftp://lpsvsh.lps.umontreal.ca/hep_th/dpf.ps . To appear as a chapter in "Electroweak Symmetry Breaking and Beyond the Standard Model", edited by T. Barklow, S. Dawson, H.E. Haber and S. Siegrist, World Scientifi

    Connected to Culture, Conformed to Christ: Exploring Alternate Forms of Worship

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    Mission on Autopilot: The Untold Story

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    Seventh-day Adventist Mission: The Shifting Landscape

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    Edge states in Open Antiferromagnetic Heisenberg Chains

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    In this letter we report our results in investigating edge effects of open antiferromagnetic Heisenberg spin chains with spin magnitudes S=1/2,1,3/2,2S=1/2, 1,3/2,2 using the density-matrix renormalization group (DMRG) method initiated by White. For integer spin chains, we find that edge states with spin magnitude Sedge=S/2S_{edge}=S/2 exist, in agreement with Valence-Bond-Solid model picture. For half-integer spin chains, we find that no edge states exist for S=1/2S=1/2 spin chain, but edge state exists in S=3/2S=3/2 spin chain with Sedge=1/2S_{edge}=1/2, in agreement with previous conjecture by Ng. Strong finite size effects associated with spin dimmerization in half-integer spin chains will also be discussed.Comment: 4 pages, RevTeX 3.0, 5 figures in a separate uuencoded postscript file. Replaced once to enlarge the acknowlegement

    From computation to black holes and space-time foam

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    We show that quantum mechanics and general relativity limit the speed ν~\tilde{\nu} of a simple computer (such as a black hole) and its memory space II to \tilde{\nu}^2 I^{-1} \lsim t_P^{-2}, where tPt_P is the Planck time. We also show that the life-time of a simple clock and its precision are similarly limited. These bounds and the holographic bound originate from the same physics that governs the quantum fluctuations of space-time. We further show that these physical bounds are realized for black holes, yielding the correct Hawking black hole lifetime, and that space-time undergoes much larger quantum fluctuations than conventional wisdom claims -- almost within range of detection with modern gravitational-wave interferometers.Comment: A misidentification of computer speeds is corrected. Our results for black hole computation now agree with those given by S. Lloyd. All other conclusions remain unchange

    Time Uncertainty in Quantum Gravitational Systems

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    It is generally argued that the combined effect of Heisenberg principle and general relativity leads to a minimum time uncertainty. Most of the analyses supporting this conclusion are based on a perturbative approach to quantization. We consider a simple family of gravitational models, including the Einstein-Rosen waves, in which the (non-linearized) inclusion of gravity changes the normalization of time translations by a monotonic energy-dependent factor. In these circumstances, it is shown that a maximum time resolution emerges non-perturbatively only if the total energy is bounded. Perturbatively, however, there always exists a minimum uncertainty in the physical time.Comment: (4 pages, no figures) Accepted for publication in Physical Review

    Frustrated multiband superconductivity

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    We show that a clean multiband superconductor may display one or several phase transitions with increasing temperature from or to frustrated configurations of the relative phases of the superconducting order parameters. These transitions may occur when more than two bands are involved in the formation of the superconducting phase and when the number of repulsive interband interactions is odd. These transitions are signalled by slope changes in the temperature dependence of the superconducting gaps.Comment: 5 pages, 3 figure
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