306 research outputs found

    A quantum group version of quantum gauge theories in two dimensions

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    For the special case of the quantum group SLq(2,C) (q=expπi/r, r3)SL_q (2,{\bf C})\ (q= \exp \pi i/r,\ r\ge 3) we present an alternative approach to quantum gauge theories in two dimensions. We exhibit the similarities to Witten's combinatorial approach which is based on ideas of Migdal. The main ingredient is the Turaev-Viro combinatorial construction of topological invariants of closed, compact 3-manifolds and its extension to arbitrary compact 3-manifolds as given by the authors in collaboration with W. Mueller.Comment: 6 pages (plain TeX

    Optimasi Portofolio Resiko Menggunakan Model Markowitz MVO Dikaitkan dengan Keterbatasan Manusia dalam Memprediksi Masa Depan dalam Perspektif Al-Qur`an

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    Risk portfolio on modern finance has become increasingly technical, requiring the use of sophisticated mathematical tools in both research and practice. Since companies cannot insure themselves completely against risk, as human incompetence in predicting the future precisely that written in Al-Quran surah Luqman verse 34, they have to manage it to yield an optimal portfolio. The objective here is to minimize the variance among all portfolios, or alternatively, to maximize expected return among all portfolios that has at least a certain expected return. Furthermore, this study focuses on optimizing risk portfolio so called Markowitz MVO (Mean-Variance Optimization). Some theoretical frameworks for analysis are arithmetic mean, geometric mean, variance, covariance, linear programming, and quadratic programming. Moreover, finding a minimum variance portfolio produces a convex quadratic programming, that is minimizing the objective function ðð¥with constraintsð ð 𥠥 ðandð´ð¥ = ð. The outcome of this research is the solution of optimal risk portofolio in some investments that could be finished smoothly using MATLAB R2007b software together with its graphic analysis

    CMS physics technical design report : Addendum on high density QCD with heavy ions

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    Зомета в терапии рака предстательной железы с метастатическим поражением костей на фоне андрогенной депривации (результаты Российского многоцентрового исследования)

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    Introduction: Hormonal therapy is the method of choice in treating disseminated prostate cancer. Chronic androgenic suppression causes a reduction in bone mineral density. The most common complications of bone metastases are pathological fractures, spinal cord compression, pain, etc.Methods: A multicenter study (11 clinics of Russia) assessing the efficacy of Zometa in preventing skeletal complications of bone metastases was conducted in 2004—2005. Zometa was administered intravenously at a dose of 4 mg every 3Р4 weeks with androgenic deprivation. Its objective effect was evaluated in 70 patients. Changes in bone mineral density were evaluated by densitometry.Results: Complete pain relief was achieved in 73% of the patients; after therapy 86% of the patients had 0—1 WHO activity status score, 97% of the patients had no bone complications. The level of bone resorption marker β-Cross-Laps decreased to the normal values in 51% of the patients.Conclusion: The study has provided an evidence of the efficacy of Zometa and the necessity of using this drug in complex therapy for bone metastases of prostate cancer.Introduction: Hormonal therapy is the method of choice in treating disseminated prostate cancer. Chronic androgenic suppression causes a reduction in bone mineral density. The most common complications of bone metastases are pathological fractures, spinal cord compression, pain, etc.Methods: A multicenter study (11 clinics of Russia) assessing the efficacy of Zometa in preventing skeletal complications of bone metastases was conducted in 2004—2005. Zometa was administered intravenously at a dose of 4 mg every 3Р4 weeks with androgenic deprivation. Its objective effect was evaluated in 70 patients. Changes in bone mineral density were evaluated by densitometry.Results: Complete pain relief was achieved in 73% of the patients; after therapy 86% of the patients had 0—1 WHO activity status score, 97% of the patients had no bone complications. The level of bone resorption marker β-Cross-Laps decreased to the normal values in 51% of the patients.Conclusion: The study has provided an evidence of the efficacy of Zometa and the necessity of using this drug in complex therapy for bone metastases of prostate cancer

    Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC

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    Azimuthal separation in nearly back-to-back jet topologies in inclusive 2-and 3-jet events in pp collisions at root s=13TeV

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    A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, Delta phi(12), is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 fb(-1) are used. Predictions based on calculations using matrix elements at leading-order and next-to-leading-order accuracy in perturbative quantum chromodynamics supplemented with leading-log parton showers and hadronization are generally in agreement with themeasurements. Discrepancies between the measurement and theoretical predictions are as large as 15%, mainly in the region 177 degrees <Delta phi(12) <180 degrees. The 2- and 3-jet measurements are not simultaneously described by any of models.Peer reviewe

    Electroweak production of two jets in association with a Z boson in proton-proton collisions root s =13 TeV

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    A measurement of the electroweak (EW) production of two jets in association with a Z boson in proton-proton collisions at root s = 13 TeV is presented, based on data recorded in 2016 by the CMS experiment at the LHC corresponding to an integrated luminosity of 35.9 fb(-1). The measurement is performed in the lljj final state with l including electrons and muons, and the jets j corresponding to the quarks produced in the hard interaction. The measured cross section in a kinematic region defined by invariant masses m(ll) > 50 GeV, m(jj) > 120 GeV, and transverse momenta P-Tj > 25 GeV is sigma(EW) (lljj) = 534 +/- 20 (stat) fb (syst) fb, in agreement with leading-order standard model predictions. The final state is also used to perform a search for anomalous trilinear gauge couplings. No evidence is found and limits on anomalous trilinear gauge couplings associated with dimension-six operators are given in the framework of an effective field theory. The corresponding 95% confidence level intervals are -2.6 <cwww/Lambda(2) <2.6 TeV-2 and -8.4 <cw/Lambda(2) <10.1 TeV-2. The additional jet activity of events in a signal-enriched region is also studied, and the measurements are in agreement with predictions.Peer reviewe

    Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at root s=13 TeV

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    Observation of the χb1(3P)\chi_{b1}(3P) and χb2(3P)\chi_{b2}(3P) and measurement of their masses

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    The χb1(3P)\chi_{b1}(3P) and χb2(3P)\chi_{b2}(3P) states are observed through their γ(3S)γ\gamma(3S)_\gamma decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 80.0  fb180.0  fb^{−1}. Theγ(3S)\gamma(3S) mesons are identified through their dimuon decay channel, while the low-energy photons are detected after converting to e+ee^+e ^− pairs in the silicon tracker, leading to a χb1(3P)\chi_{b1}(3P) mass resolution of 2.2 MeV. This is the first time that the J=1 and 2 states are well resolved and their masses individually measured: 10513.42±0.41(stat)±0.18(syst)  MeV10513.42±0.41(stat)±0.18(syst)  MeV and 10524.02±0.57(stat)±0.18(syst)  MeV10524.02±0.57(stat)±0.18(syst)  MeV; they are determined with respect to the world-average value of the γ(3S)\gamma(3S) mass, which has an uncertainty of 0.5 MeV. The mass splitting is measured to be 10.60±0.64(stat)±0.17(syst)  MeV10.60±0.64(stat)±0.17(syst)  MeV
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