963 resultados para University of Minnesota
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Back Row: James Johns, Irwin Uteritz, Harold MacGregor, John Gunther, Waldeck Levi, Homer(?) Martin, Charles Kreis, Stephen Garfield, Walter Kreinheder, Frank Culver, Herndon Taylor, Walter Dean, John Perrin, Herbert Dunphy, ? McWood, assistant coach Angus Goetz, Frederick Novy, Paul Goebel, Stan Muirhead, Edward Usher, Leroy Neisch, assistant coach Elton Wieman, assistant coach A.J. Sturznegger
Front Row: Verne Richards, Oscar Olson, Louis Curran, William Crawforth, Harry Kipke, John Searle, Franklin Cappon, Theodore Banks, John Evans, John Keatley, Donald Hathaway, John Fairbairn, J.W. McAuliffe, John Landowski, Alexander Oliver, Donald Swan, Douglas Roby, Bernard Kirk, Robert Jerome Dunne, trasiner Archie Hahn, Leroy Neisch
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Back Row, standing: Harold Ackershook, Ira Grinnell, Roy Hudson, Karl Richardson, Leslie Avery, Fielding H. Yost, jr., Hilbert Horwitz, Robert C. Morgan, Maynard Morrison, Thomas Samuels, Estel Tessmer, Russell Damm, Claire Purdum, Sylvester Shea, Ivan Williamson, Stanley Hozer, Roderick Cox, William Gitman, William Jordan, Ward Oehman, Ivan Smith, Carl Castle, Omer LaJeuness, Leo Draveling, Howard Auer
Middle Row: Francis Cornwell, Oscar Lundin, Jay Sikkenga, Charles DeBaker, Leslie Frisk, Norman Daniels, Harry Newman, George Bremen, William Unger, Thomas Justice, Kenneth Manuel, Orville Parker, Walfred Kuijala, Robert (?)Hayes, Keith(?) Tyler, Leslie Douglass, DuVal Goldsmith
Front Row: Emmett O'Neill, Claude Stoll, Clare Jack Wheeler, Ward O'Neill, James Simrall, Aber Marcovksy, Alber Berkowitz, Harry Eastman, William M. Heston jr., Arthur Podlewski, J. Charles Markley, Ralph Wills, Harold Lindsay, William Benz, Arthur Kutsche, Harry(?) Benjamin, J. Leo Winston, William Hewitt
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Back Row: Dennis Youngblood, William Pratt, C. Robert Johnson, Robert Callahan, Jack Weisenburger, Russell Reader, Gene Hinton, Robert Swanson, Stanley Kuick, Robert Allen Wahl, Anton Momsen, Daniel Dworsky, F. Stuart Wilkins, Reginald Sauls
3rd Row: Walter Teninga, Horace Coleman, George Chiames, John Lintol, George Johnson, John Anderson, Donovan Hershberger, Edward McNeill, John Smith, Peter Elliott, John Ott, Michael Prashaw
2nd Row: James Foltz, Louis Brunsting, Russell Kavanaugh, Howard Yerges, Harold Watts, Joseph Ponsetto, Frank Nakamura, Joseph Soboleski, Carl Freihofer, John Weyers, Dominic Tomasi
Front Row: George Hutter, Norman Rabbers, Henry Fonde, Howard Doty, Edward Grenkoski, Warren Bentz, Wesley Muelder, William Redmond
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Mimeographed.
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Mode of access: Internet.
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Although malaria in Brazil almost exclusively occurs within the boundaries of the Amazon Region, some concerns are raised regarding imported malaria to non-endemic areas of the country, notably increased incidence of complications due to delayed diagnoses. However, although imported malaria in Brazil represents a major health problem, only a few studies have addressed this subject. A retrospective case series is presented in which 263 medical charts were analysed to investigate the clinical and epidemiological characterization of malaria cases that were diagnosed and treated at Hospital & Clinics, State University of Campinas between 1998 and 2011. Amongst all medical charts analysed, 224 patients had a parasitological confirmed diagnosis of malaria. Plasmodium vivax and Plasmodium falciparum were responsible for 67% and 30% of the infections, respectively. The majority of patients were male (83%) of a productive age (median, 37 years old). Importantly, severe complications did not differ significantly between P. vivax (14 cases, 9%) and P. falciparum (7 cases, 10%) infections. Severe malaria cases were frequent among imported cases in Brazil outside of the Amazon area. The findings reinforce the idea that P. vivax infections in Brazil are not benign, regardless the endemicity of the area studied. Moreover, as the hospital is located in a privileged site, it could be used for future studies of malaria relapses and primaquine resistance mechanisms. Finally, based on the volume of cases treated and the secondary complications, referral malaria services are needed in the non-endemic areas of Brazil for a rapid and efficient and treatment.
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The magnetized MINOS Near Detector, at a depth of 225 mwe, is used to measure the atmospheric muon charge ratio. The ratio of observed positive to negative atmospheric muon rates, using 301 days of data, is measured to be 1.266 +/- 0.001(stat)(-0.014)(+0.015)(syst). This measurement is consistent with previous results from other shallow underground detectors and is 0.108 +/- 0.019(stat + syst) lower than the measurement at the functionally identical MINOS Far Detector at a depth of 2070 mwe. This increase in charge ratio as a function of depth is consistent with an increase in the fraction of muons arising from kaon decay for increasing muon surface energies.
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This Letter reports the first direct observation of muon antineutrino disappearance. The MINOS experiment has taken data with an accelerator beam optimized for (nu) over bar (mu) production, accumulating an exposure of 1.71 x 10(20) protons on target. In the Far Detector, 97 charged current (nu) over bar (mu) events are observed. The no-oscillation hypothesis predicts 156 events and is excluded at 6.3 sigma. The best fit to oscillation yields vertical bar Delta(m) over bar (2)vertical bar = [3.36(-0.40)(+0.46)(stat) +/- 0.06(sys)] x 10(-3) eV(2), sin(2)(2 (theta) over bar) = 0.86(-0.12)(+0.11)(stat) +/- 0.01(syst). The MINOS nu(mu) and (nu) over bar (mu) measurements are consistent at the 2.0% confidence level, assuming identical underlying oscillation parameters.
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This Letter reports new results from the MINOS experiment based on a two-year exposure to muon neutrinos from the Fermilab NuMI beam. Our data are consistent with quantum-mechanical oscillations of neutrino flavor with mass splitting vertical bar Delta m(2)vertical bar = (2.43 +/- 0.13) x 10(-3) eV(2) (68% C.L.) and mixing angle sin(2)(2 theta) > 0.90 (90% C.L.). Our data disfavor two alternative explanations for the disappearance of neutrinos in flight: namely, neutrino decays into lighter particles and quantum decoherence of neutrinos, at the 3.7 and 5.7 standard-deviation levels, respectively.
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Measurements of neutrino oscillations using the disappearance of muon neutrinos from the Fermilab NuMI neutrino beam as observed by the two MINOS detectors are reported. New analysis methods have been applied to an enlarged data sample from an exposure of 7.25 x 10(20) protons on target. A fit to neutrino oscillations yields values of vertical bar Delta m(2)vertical bar = (2.32(-0.08)(+0.12) x 10(-3) eV(2) for the atmospheric mass splitting and sin(2)(2 theta) > 0.90 (90% C.L.) for the mixing angle. Pure neutrino decay and quantum decoherence hypotheses are excluded at 7 and 9 standard deviations, respectively.
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We consider a class of two-dimensional problems in classical linear elasticity for which material overlapping occurs in the absence of singularities. Of course, material overlapping is not physically realistic, and one possible way to prevent it uses a constrained minimization theory. In this theory, a minimization problem consists of minimizing the total potential energy of a linear elastic body subject to the constraint that the deformation field must be locally invertible. Here, we use an interior and an exterior penalty formulation of the minimization problem together with both a standard finite element method and classical nonlinear programming techniques to compute the minimizers. We compare both formulations by solving a plane problem numerically in the context of the constrained minimization theory. The problem has a closed-form solution, which is used to validate the numerical results. This solution is regular everywhere, including the boundary. In particular, we show numerical results which indicate that, for a fixed finite element mesh, the sequences of numerical solutions obtained with both the interior and the exterior penalty formulations converge to the same limit function as the penalization is enforced. This limit function yields an approximate deformation field to the plane problem that is locally invertible at all points in the domain. As the mesh is refined, this field converges to the exact solution of the plane problem.
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The thermoelastic properties of ferropericlase Mg(1-x)Fe(x)O (x = 0.1875) throughout the iron high-to-low spin cross-over have been investigated by first principles at Earth`s lower mantle conditions. This cross-over has important consequences for elasticity such as an anomalous bulk modulus (K(S)) reduction. At room temperature the anomaly is somewhat sharp in pressure but broadens with increasing temperature. Along a typical geotherm it occurs across most of the lower mantle with a more significant K(S) reduction at approximate to 1,400-1,600 km depth. This anomaly might also cause a reduction in the effective activation energy for diffusion creep and lead to a viscosity minimum in the mid-lower mantle, in apparent agreement with results from inversion of data related with mantle convection and postglacial rebound.
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As seen from Blair Road.
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As seen from Balir Road.
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Formal elevation facing University of Queensland entrance roads.