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7081por Fukuhara, Mikio“…The H and He atoms produced and the anti-neutrino [Image: see text] are incorporated as Fe-H based alloys in the H-rich portion of inner core, are released from Earth’s interior to the universe, and pass through Earth, respectively.…”
Publicado 2016
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7082por Niemes, Simon, Telle, Helmut H., Bornschein, Beate, Fasselt, Lucian, Größle, Robin, Priester, Florian, Schlösser, Magnus, Sturm, Michael, Welte, Stefan, Zeller, Genrich“…Highly accurate, quantitative analyses of mixtures of hydrogen isotopologues—both the stable species, H(2), D(2), and HD, and the radioactive species, T(2), HT, and DT—are of great importance in fields as diverse as deuterium–tritium fusion, neutrino mass measurements using tritium β-decay, or for photonuclear experiments in which hydrogen–deuterium targets are used. …”
Publicado 2021
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7083por Jwa, Yeon-jae, Di Guglielmo, Giuseppe, Arnold, Lukas, Carloni, Luca, Karagiorgi, Georgia“…We use “High Level Synthesis for Machine Learning” (hls4ml) tools to test CNN deployment on a Xilinx UltraScale+ FPGA, which is an FPGA technology proposed for use in the front-end readout system of the future Deep Underground Neutrino Experiment (DUNE) particle detector. We evaluate network accuracy and estimate latency and hardware resource usage, and comment on the feasibility of applying CNNs for real-time data selection within the currently planned DUNE data acquisition system. …”
Publicado 2022
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7084por Abbiendi, G., Ackerstaff, K., Alexander, G., Allison, John, Altekamp, N., Anderson, K.J., Anderson, S., Arcelli, S., Asai, S., Ashby, S.F., Axen, D., Azuelos, G., Ball, A.H., Barberio, E., Barlow, Roger J., Batley, J.R., Baumann, S., Bechtluft, J., Behnke, T., Bell, Kenneth Watson, Bella, G., Bellerive, A., Bentvelsen, S., Bethke, S., Betts, S., Biebel, O., Biguzzi, A., Blobel, V., Bloodworth, I.J., Bock, P., Bohme, J., Bonacorsi, D., Boutemeur, M., Braibant, S., Bright-Thomas, P., Brigliadori, L., Brown, Robert M., Burckhart, H.J., Capiluppi, P., Carnegie, R.K., Carter, A.A., Carter, J.R., Chang, C.Y., Charlton, David G., Chrisman, D., Ciocca, C., Clarke, P.E.L., Clay, E., Cohen, I., Conboy, J.E., Cooke, O.C., Couyoumtzelis, C., Coxe, R.L., Cuffiani, M., Dado, S., Dallavalle, G.Marco, Davis, R., De Jong, S., de Roeck, A., Dervan, P., Desch, K., Dienes, B., Dixit, M.S., Dubbert, J., Duchovni, E., Duckeck, G., Duerdoth, I.P., Estabrooks, P.G., Etzion, E., Fabbri, F., Fanfani, A., Fanti, M., Faust, A.A., Fiedler, F., Fierro, M., Fleck, I., Folman, R., Frey, A., Furtjes, A., Futyan, D.I., Gagnon, P., Gary, J.W., Gascon, J., Gascon-Shotkin, S.M., Gaycken, G., Geich-Gimbel, C., Giacomelli, G., Giacomelli, P., Gibson, V., Gibson, W.R., Gingrich, D.M., Glenzinski, D., Goldberg, J., Gorn, W., Grandi, C., Graham, K., Gross, E., Grunhaus, J., Gruwe, M., Hanson, G.G., Hansroul, M., Hapke, M., Harder, K., Harel, A., Hargrove, C.K., Hauschild, M., Hawkes, C.M., Hawkings, R., Hemingway, R.J., Herndon, M., Herten, G., Heuer, R.D., Hildreth, M.D., Hill, J.C., Hobson, P.R., Hoch, M., Hocker, James Andrew, Hoffman, Kara Dion, Homer, R.J., Honma, A.K., Horvath, D., Hossain, K.R., Howard, R., Huntemeyer, P., Igo-Kemenes, P., Imrie, D.C., Ishii, K., Jacob, F.R., Jawahery, A., Jeremie, H., Jimack, M., Jones, C.R., Jovanovic, P., Junk, T.R., Kanzaki, J., Karlen, D., Kartvelishvili, V., Kawagoe, K., Kawamoto, T., Kayal, P.I., Keeler, R.K., Kellogg, R.G., Kennedy, B.W., Kim, D.H., Klier, A., Kobayashi, T., Kobel, M., Kokott, T.P., Kolrep, M., Komamiya, S., Kowalewski, Robert V., Kress, T., Krieger, P., von Krogh, J., Kuhl, T., Kyberd, P., Lafferty, G.D., Landsman, H., Lanske, D., Lauber, J., Lautenschlager, S.R., Lawson, I., Layter, J.G., Lee, A.M., Lellouch, D., Letts, J., Levinson, L., Liebisch, R., List, B., Littlewood, C., Lloyd, A.W., Lloyd, S.L., Loebinger, F.K., Long, G.D., Losty, M.J., Lu, J., Ludwig, J., Lui, D., Macchiolo, A., Macpherson, A., Mader, W., Mannelli, M., Marcellini, S., Markopoulos, C., Martin, A.J., Martin, J.P., Martinez, G., Mashimo, T., Mattig, Peter, McDonald, W.John, McKenna, J., Mckigney, E.A., McMahon, T.J., McPherson, R.A., Meijers, F., Menke, S., Merritt, F.S., Mes, H., Meyer, J., Michelini, A., Mihara, S., Mikenberg, G., Miller, D.J., Mir, R., Mohr, W., Montanari, A., Mori, T., Nagai, K., Nakamura, I., Neal, H.A., Nisius, R., O'Neale, S.W., Oakham, F.G., Odorici, F., Ogren, H.O., Oreglia, M.J., Orito, S., Palinkas, J., Pasztor, G., Pater, J.R., Patrick, G.N., Patt, J., Perez-Ochoa, R., Petzold, S., Pfeifenschneider, P., Pilcher, J.E., Pinfold, J., Plane, David E., Poffenberger, P., Poli, B., Polok, J., Przybycien, M., Rembser, C., Rick, H., Robertson, S., Robins, S.A., Rodning, N., Roney, J.M., Rosati, S., Roscoe, K., Rossi, A.M., Rozen, Y., Runge, K., Runolfsson, O., Rust, D.R., Sachs, K., Saeki, T., Sahr, O., Sang, W.M., Sarkisian, E.K.G., Sbarra, C., Schaile, A.D., Schaile, O., Scharff-Hansen, P., Schieck, J., Schmitt, S., Schoning, A., Schroder, Matthias, Schumacher, M., Schwick, C., Scott, W.G., Seuster, R., Shears, T.G., Shen, B.C., Shepherd-Themistocleous, C.H., Sherwood, P., Siroli, G.P., Sittler, A., Skuja, A., Smith, A.M., Snow, G.A., Sobie, R., Soldner-Rembold, S., Spagnolo, S., Sproston, M., Stahl, A., Stephens, K., Steuerer, J., Stoll, K., Strom, David M., Strohmer, R., Surrow, B., Talbot, S.D., Taras, P., Tarem, S., Teuscher, R., Thiergen, M., Thomas, J., Thomson, M.A., Torrence, E., Towers, S., Trigger, I., Trocsanyi, Z., Tsur, E., Turcot, A.S., Turner-Watson, M.F., Ueda, I., Van Kooten, Rick J., Vannerem, P., Verzocchi, M., Voss, H., Wackerle, F., Wagner, A., Ward, C.P., Ward, D.R., Watkins, P.M., Watson, A.T., Watson, N.K., Wells, P.S., Wermes, N., White, J.S., Wilson, G.W., Wilson, J.A., Wyatt, T.R., Yamashita, S., Yekutieli, G., Zacek, V., Zer-Zion, D.“…The complementary decay mode of the scalar top quark decaying into a bottom quark, a charged lepton and a scalar neutrino has also been studied. From a search for the scalar bottom quark, a mass limit of 88.6 GeV was obtained if the mass difference between the scalar bottom quark and the lightest neutralino is larger than 7 GeV. …”
Publicado 1999
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7085por Albrecht, Johannes“…The last presented probe extensions to the SM is the search for Majorana neutrinos in same sign decays of $B^+ \to h^{-}\mu^{+}\mu^{1}$ where $h^{-}$ represents a $K^{-}$ or $\pi^{-}$. …”
Publicado 2011
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7086por Bronner, Johanna“…The vector boson fusion production rate of the Standard Model Higgs boson has been measured in decays into two $W$ bosons, each subsequently decaying into an electron or muon and a neutrino, with the ATLAS detector at the Large Hadron Collider (LHC). …”
Publicado 2014
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7087por Close, Frank“…Bruno Pontecorvo dedicated his career to hunting for the Higgs boson of his day: the neutrino, a nearly massless particle considered essential to the process of nuclear fission. …”
Publicado 2015
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7088por Jansen, H, Alvarez Sanchez, P, Bart Pedersen, S, Dehning, B, Dobos, D, Effinger, E, Ferrari, A, Griesmayer, E, Gschwendtner, E, Kozsar, I, Missiaen, D, Pernegger, H, Sala, P.R, Serrano, J, Ward, C“…A new fast diagnostic tool was installed in the CNGS facility in 2011 following the neutrino time-of-flight results published by OPERA in September 2011. …”
Publicado 2013
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7089por WENNINGER, Horst“…Career summary 1965 Ph.D. thesis work in nuclear physics at the University of Heidelberg 1968 Staff member CERN, Geneva, Switzerland: Big European Bubble Chamber (BEBC) project 1981 Leader of BEBC Group at CERN 1984 Leader of Experimental Facility Division (EF) at CERN 1990 Leader of Accelerator Technology Division (AT/LHC) at CERN 1993 LHC Deputy Project Leader at CERN 1994 Research/Technical Director at CERN 2000 -2003 R&D superconducting RF cavities CERN-DESY /CERN Future Since 1982 Member of various boards (BMBF Bonn, DESY, GSI, Jülich) 1997-2000 Chairman of Scientific Advisory Board, Helsinki Institute of Physics 2000 – 2004 Member of Scientific Review Group for Norwegian Research Council 2000 – 2013 Member of Technology Panel, European Physical Society 2005 - 2013 Facility for Antiproton Ion Research, GSI Activities: Nuclear physics spectroscopy, bubble chamber physics, neutrino physics, LEP physics experiments, particle physics detector and accelerator R&D …”
Publicado 2014
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7090por Laporte, Jean-Francois“…The nucleon strange density plays an important role for a number of physics processes, including the formation of strange matter and neutrino interactions at ultrahigh energies. The precision measurements of inclusive W and Z production as well as the production of W bosons in association with a charm quark provide new constraints on the strange density in the proton. …”
Publicado 2014
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7091por Dalchenko, Mykhailo“…Constraints on the Higgs boson width were established using its off-shell production and decay to a pair of $Z$ bosons, where one $Z$ boson decays to an electron or muon pair, and the other to an electron, muon, or neutrino pair. The obtained result is an upper limit on the Higgs boson width of $22~$MeV at a 95% confidence level, which is 5.4 times the expected value in the standard model at the measured mass. …”
Publicado 2015
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7092“…A thorough account is given of quark flavour and neutrino oscillations based on published experimental results, including some from running experiments. …”
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7093por Tsirintanis, Nikolaos“…The existence of new heavy charged vector bosons is investigated in events containing a muon and neutrino pair. Neutrinos are observed indirectly via the presence of high missing transverse energy. …”
Publicado 2016
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7094por Faulkner, James Anthony“…The W boson decays leptonically to an electron or muon, or their respective antiparticle, paired with the appropriate neutrino. The second boson V decays hadronically into two jets, and additionally a photon is required in the event. …”
Publicado 2016
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7095
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7096por Marley, Daniel Edison“…The first analysis considers final states with 1-lepton and hadronic jets that can be used to reconstruct the vector-like quark system after identifying the boosted decay of $W$ bosons and building the neutrino from the missing transverse momentum. Control and signal regions constrain the uncertainties associated with $t\bar{t}$ production that most negatively impact this analysis. …”
Publicado 2017
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7097por Burger, Angela Maria“…The electron identification efficiency and its uncertainty is also an important input to the measurement of $WZ$ production using fully leptonic decays to electrons, muons and a neutrino. Measurements of the $WZ$ production are sensitive to the $WWZ$ vector boson coupling. …”
Publicado 2018
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7098por Dascalau, Titus, Flowerdew, Jake, Griffin-Hicks, Peter, Hughes, Adam, Mussolini, Carlo Alberto, Pakuza, Collette, Topp-Mugglestone, Max, Wang, Wei-Ting, Wroe, Laurence“…Radiation deposition in the accelerator was also investigated, along with a study on the environmental exposure from neutrino radiation.…”
Publicado 2020
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7099por Muller, Denise“…In the search, leptonically decaying top quarks are analyzed, resulting in a final state of the signal process consisting of one charged muon or electron and its corresponding neutrino, and two jets originating from hadronized bottom quarks. …”
Publicado 2020
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7100por Pepe-Altarelli, Monica“…In 1987 she joined CERN as research fellow in the ALEPH experiment at the LEP accelerator; she was one of the principal authors of the first measurement of the number of light neutrino species, one of the main results of LEP, in a small group led by Jack Steinberger. …”
Publicado 2022
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