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  1. 20681
    por Önengüt, G, Van Dantzig, R, De Jong, M, Oldeman, R G C, Güler, M, Köse, U, Tolun, P, Catanesi, M G, Muciaccia, M T, Winter, Klaus, Van de Vyver, B, Vilain, P, Wilquet, G, Saitta, B, Di Capua, E, Ogawa, S, Shibuya, H, Goldberg, J, Hristova, I R, Kawamura, T, Kolev, D, Kayis-Topaksu, A, Meinhard, H, Panman, J, Rozanov, A, Tsenov, R V, Zucchelli, P, Uiterwijk, J W E, Chikawa, M, Song, J S, Yoon, C S, Kodama, K, Ushida, N, Hara, T, Aoki, S, Delbar, T, Favart, D, Grégoire, G, Kalinin, S, Makhlyoueva, I V, Bruski, N, Frekers, D, Tsukerman, I, Shamanov, V V, Khovanskii, V D, Gorbunov, P, Artamonov, A V, Sato, Y, Tezuka, I, Barbuto, E, Bozza, C, Grella, G, Romano, G, Sirignano, C, Sorrentino, S, Dore, U, Loverre, P F, Ludovici, L, Rosa, G, Santacesaria, R, Satta, A, Spada, F R, Okusawa, T, Hoshino, K, Kawada, J, Komatsu, M, Miyanishi, M, Nakamura, M, Nakano, T, Narita, K, Niu, K, Niwa, K, Nonaka, N, Sato, O, Toshito, T, Buontempo, S, Cocco, A G, D'Ambrosio, N, De Lellis, G, De Rosa, G, Di Capua, F, Fiorillo, G, Marotta, A, Messina, M, Migliozzi, P, Scotto-Lavina, L, Strolin, P, Tioukov, V
    Publicado 2005
    “…During the years 1994-97, the emulsion target of the CHORUS detector was exposed to the wide-band neutrino beam of the CERN SPS of 27 GeV average neutrino energy. In total about 100 000 charged-current neutrino interactions were located in the nuclear emulsion target and fully reconstructed. …”
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    Measurement of $D^{*+}$ production in charged-current neutrino interactions
  2. 20682
    por Kayis-Topaksu, A, Önengüt, G, Van Dantzig, R, De Jong, M, Oldeman, R G C, Güler, M, Köse, U, Tolun, P, Catanesi, M G, Muciaccia, M T, Winter, Klaus, Van de Vyver, B, Vilain, P, Wilquet, G, Saitta, B, Di Capua, E, Ogawa, S, Shibuya, H, Hristova, I R, Kawamura, T, Kolev, D, Meinhard, H, Panman, J, Rozanov, A, Tsenov, R V, Uiterwijk, J W E, Zucchelli, P, Goldberg, J, Chikawa, M, Song, J S, Yoon, C S, Kodama, K, Ushida, N, Aoki, S, Hara, T, Delbar, T, Favart, D, Grégoire, G, Kalinin, S, Makhlyoueva, I V, Artamonov, A V, Gorbunov, P, Khovanskii, V D, Shamanov, V V, Tsukerman, I, Bruski, N, Frekers, D, Hoshino, K, Kawada, J, Komatsu, M, Myanishi, M, Nakamura, M, Nakano, T, Narita, K, Niu, K, Niwa, K, Nonaka, N, Sato, O, Toshito, T, Buontempo, S, Cocco, A G, D'Ambrosio, N, De Lellis, G, De Rosa, G, Di Capua, F, Fiorillo, G, Marotta, A, Messina, M, Migliozzi, P, Scotto-Lavina, L, Strolin, P, Tioukov, V, Okusawa, T, Dore, U, Loverre, P F, Ludovici, L, Rosa, G, Santacesaria, R, Satta, A, Spada, F R, Barbuto, E, Bozza, C, Grella, G, Romano, G, Sirignano, C, Sorrentino, S, Sato, Y, Tezuka, I
    Publicado 2005
    “…Selecting only events with visible energy greater than 30 GeV gives a value of Bμ that is less affected by the charm production threshold and quasi-elastic _+ c production. …”
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    Measurement of topological muonic branching ratios of charmed hadrons produced in neutrino-induced charged-current interactions
  3. 20683
    por Mitrovski, Michael K., Alt, C., Anticic, T., Baatar, B., Barna, D., Bartke, J., Betev, L., Bialkowska, H., Blume, C., Boimska, B., Botje, M., Bracinik, J., Bramm, R., Buncic, P., Cerny, V., Christakoglou, P., Chung, P., Chvala, O., Cramer, J.G., Csato, P., Dinkelaker, P., Eckardt, V., Flierl, D., Fodor, Z., Foka, P., Friese, V., Gal, J., Gazdzicki, M., Genchev, V., Georgopoulos, G., Gladysz, E., Grebieszkow, K., Hegyi, S., Hohne, C., Kadija, K., Karev, A., Kikola, D., Kliemant, M., Kniege, S., Kolesnikov, V.I., Kornas, E., Korus, R., Kowalski, M., Kraus, I., Kreps, M., Laszlo, A., Lacey, R., van Leeuwen, M., Levai, P., Litov, L., Lungwitz, B., Makariev, M., Malakhov, A.I., Mateev, M., Melkumov, G.L., Meurer, C., Mischke, A., Molnar, J., Mrowczynski, St., Nicolic, V., Palla, G., Panagiotou, A.D., Panayotov, D., Petridis, A., Peryt, W., Pikna, M., Pluta, J., Prindle, D., Puhlhofer, F., Renfordt, R., Roland, C., Roland, G., Rybczynski, M., Rybicki, A., Sandoval, A., Schmitz, N., Schuster, T., Seyboth, P., Sikler, F., Sitar, B., Skrzypczak, E., Slodkowski, M., Stefanek, G., Stock, R., Strabel, C., Strobele, H., Susa, T., Szentpetery, I., Sziklai, J., Szuba, M., Szymanski, P., Trubnikov, V., Varga, D., Vassiliou, M., Veres, G.I., Vesztergombi, G., Vranic, D., Wetzler, A., Wlodarczyk, Z., Yoo, I.K., Zimanyi, J.
    Publicado 2006
    “…We present a summary of measurements of strange particles performed by the experiment NA49 in central and minimum bias Pb+Pb collisions in the beam energy range 20A - 158A GeV. New results on $\Xi$ production in central Pb+Pb collisions and on $\Lambda, \Xi$ production in minimum bias collisions are shown. …”
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    Strangeness production at SPS energies
  4. 20684
    por Kaneda, Michiru
    Publicado 2015
    “…The mini black hole signals for n = 2 to 7 and M D = 0 . 8 GeV to 2 TeV are searched for. For each n and M D , the mass thresholds of the mini black holes were set by the assumptions that colliding particles collapse in a black hole if the Compton wavelength is equal to or less than the Schwarzschild radius or horizon radius. …”
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    Search for the Mini Black Hole in the Multijet Final State in pp Collisions at √ s = 7 TeV
  5. 20685
    por Bogomilov, M, Matev, R, Tsenov, R, Dracos, M, Bonesini, M, Palladino, V, Tortora, L, Mori, Y, Planche, T, Lagrange, J  B, Kuno, Y, Benedetto, E, Efthymiopoulos, I, Garoby, R, Gilardoini, S, Martini, M, Wildner, E, Prior, G, Blondel, A, Karadzhow, Y, Ellis, M, Kyberd, P, Bayes, R, Laing, A, Soler, F  J  P, Alekou, A, Apollonio, M, Aslaninejad, M, Bontoiu, C, Jenner, L  J, Kurup, A, Long, K, Pasternak, J, Zarrebini, A, Poslimski, J, Blackmore, V, Cobb, J, Tunnell, C, Andreopoulos, C, Bennett, J  R  J, Brooks, S, Caretta, O, Davenne, T, Densham, C, Edgecock, T  R, Fitton, M, Kelliher, D, Loveridge, P, McFarland, A, Machida, S, Prior, C, Rees, G, Rogers, C, Rooney, M, Thomason, J, Wilcox, D, Booth, C, Skoro, G, Back, J  J, Harrison, P, Berg, J  S, Fernow, R, Gallardo, J  C, Gupta, R, Kirk, H, Simos, N, Stratakis, D, Souchlas, N, Witte, H, Bross, A, Geer, S, Johnstone, C, Mokhov, N, Neuffer, D, Popovic, M, Strait, J, Striganov, S, Morfín, J  G, Wands, R, Snopok, P, Bogacz, S  A, Morozov, V, Roblin, Y, Cline, D, Ding, X, Bromberg, C, Hart, T, Abrams, R  J, Ankenbrandt, C  M, Beard, K  B, Cummings, M  A  C, Flanagan, G, Johnson, R  P, Roberts, T  J, Yoshikawa, C  Y, Graves, V  B, McDonald, K  T, Coney, L, Hanson, G
    Publicado 2014
    “…The EURO$\nu$ baseline accelerator facility will provide 10$^{21}$ muon decays per year from 12.6 GeV stored muon beams serving a single neutrino detector situated at a source-detector distance of between 1500 km and 2500 km. …”
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    Neutrino Factory
  6. 20686
    por Engl, Albert
    Publicado 2016
    “…The single tube resolution of these 15 mm drift tubes was determined to be 95 m at the H8 test facility at CERN using a muon beam with an energy of 140 GeV.…”
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    Precise muon drift tube detectors for high background rate conditions
  7. 20687
    por Dräger, Arne-Rasmus
    Publicado 2016
    “…The production of light-flavor $\tilde{\text{q}}$ below a mass of 780 GeV and $\tilde{\text{g}}$ with masses below 1.1-1.2 TeV are excluded at 95\% confidence level. …”
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    Prediction of the $\text{t}\bar{\text{t}}$ and $\text{W}+\text{Jets}$ Background in a Search for New Physics with Jets and Missing Transverse Energy at CMS
  8. 20688
    “…The AD machine at European Organization for Nuclear Research (CERN) is presently being used to decelerate antiprotons from 3.57 GeV/c to 100 MeV/c for matter vs anti-matter comparative studies. …”
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    The AD and ELENA orbit, trajectory and intensity measurement systems
  9. 20689
    por Radhakrishnan, Sooraj
    Publicado 2017
    “…The ridge correlations are found to persist to high pT (⇠10 GeV). Fourier harmonics up to order 5 are measured and found to be non-zero. …”
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    Study of long-range azimuthal and longitudinal correlations in high energy nuclear collisions at the LHC using the ATLAS detector
  10. 20690
    por Lopez Paredes, Brais
    Publicado 2018
    “…It is also applied in the search for Higgs decays to a Z boson and a photon, H → Zγ, introducing a 2% improvement in the upper limit set by the analysis, yielding 11 × S M at mH = 125.5 GeV (95% CL). The method is also used in the measurement of the photon electromagnetic scale to provide a precision better than 0.5%, reducing the measured Higgs mass systematic uncertainty obtained from the H → γγ analysis. …”
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    ATLAS Electromagnetic Calorimeter performance measurements, search for the Higgs boson in the $H \to Z\gamma$ channel and detector development for position reconstruction of noble liquid scintillation
  11. 20691
    por Kovalchuk, Nataliia
    Publicado 2018
    “…The top quark mass is measured to be $m_{t} = 172.25 \pm0.08 \mbox{ (stat+JSF)}\pm0.62\mbox{ (syst) GeV}$. The results are tested for possible kinematic dependence by performing measurements of the top quark mass in different phase space regions.The residual data-to-simulation calibration of the energy of the jets is also estimated from dijet events with data collected at center-of-mass energy of 13 TeV in 2015 with the CMS detector corresponding to an integrated luminosity of 2.1 fb$^{-1}$. …”
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    Top quark mass measurement and color effects at the LHC
  12. 20692
    “…For this purpose, experiments were carried out at the CERN HiRadMat (High Radiation to Materials) facility in which extended solid copper cylindrical targets were irradiated with the 440 GeV proton beam generated by the Super Proton Synchrotron (SPS). …”
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    Review of hydrodynamic tunneling issues in high power particle accelerators
  13. 20693
    “…This paper reports a benchmarking study against beam experiments performed at the HiRadMat (High-Radiation to Materials) facility using beams at 440 GeV from the Super Proton Synchrotron. Good agreement has been found between the simulation results and the experiments as well as previous simulations with fluka and big2 [Tahir et al., Phys. …”
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    Simulation of hydrodynamic tunneling induced by high-energy proton beam in copper by coupling computer codes
  14. 20694
    por Arnold, Oliver Werner
    Publicado 2019
    “…These pairs were produced in reaction of p+Nb, where the proton had a kinetic energy of 3.5 GeV. At the beginning, all experimental correlation function were corrected for various detector effects. …”
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    Study of the hyperon-nucleon interaction via femtoscopy in elementary systems with HADES and ALICE
  15. 20695
    por Polukhina, N G, Shchedrina, T V
    Publicado 2019
    “…The SHiP experiment (for Search for Hidden Particles) which will operate at the CERN Super Proton Synchrotron (SPS) is one of the most promising projects in the field of particle physics. The SPS 400-GeV/c proton beam will be dumped onto the molybdenum–tungsten target of the SHiP detector, and the data corresponding to $2 \times 10^{20}$ protons on the target will be accumulated in five years of running. …”
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    The SHiP Experiment: Search for New Physics in the Neutrino Sector
  16. 20696
    por Heister, Arno
    Publicado 2007
    “…For quite low masses (50 < mH0 < 130[ GeV]) )1 the Higgs will predominantly decay into two b-quarks. …”
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    Development of an object oriented C++ algorithm for b-quark identification (Development of methods of b-quark identification in high energy $e^+e^-$ and pp collisions)
  17. 20697
    “…Here we study the effects of two different types of ionizing radiation (IR) treatment, HZE (1 GeV Fe(26+) high mass, high charge, and high energy relativistic particles) and gamma photons, on the transcriptome of Arabidopsis thaliana seedlings. …”
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    Online Artículo Texto
    High atomic weight, high-energy radiation (HZE) induces transcriptional responses shared with conventional stresses in addition to a core “DSB” response specific to clastogenic treatments
  18. 20698
    por Adinolfi, M., Aglieri Rinella, G., Albrecht, E., Bellunato, T., Benson, S., Blake, T., Blanks, C., Brisbane, S., Brook, N. H., Calvi, M., Cameron, B., Cardinale, R., Carson, L., Contu, A., Coombes, M., D’Ambrosio, C., Easo, S., Egede, U., Eisenhardt, S., Fanchini, E., Fitzpatrick, C., Fontanelli, F., Forty, R., Frei, C., Gandini, P., Gao, R., Garra Tico, J., Giachero, A., Gibson, V., Gotti, C., Gregson, S., Gys, T., Haines, S. C., Hampson, T., Harnew, N., Hill, D., Hunt, P., John, M., Jones, C. R., Johnson, D., Kanaya, N., Katvars, S., Kerzel, U., Kim, Y. M., Koblitz, S., Kucharczyk, M., Lambert, D., Main, A., Maino, M., Malde, S., Mangiafave, N., Matteuzzi, C., Mini’, G., Mollen, A., Morant, J., Mountain, R., Morris, J. V., Muheim, F., Muresan, R., Nardulli, J., Owen, P., Papanestis, A., Patel, M., Patrick, G. N., Perego, D. L., Pessina, G., Petrolini, A., Piedigrossi, D., Plackett, R., Playfer, S., Powell, A., Rademacker, J. H., Ricciardi, S., Rogers, G. J., Sail, P., Sannino, M., Savidge, T., Sepp, I., Sigurdsson, S., Soler, F. J. P., Solomin, A., Soomro, F., Sparkes, A., Spradlin, P., Storaci, B., Thomas, C., Topp-Joergensen, S., Torr, N., Ullaland, O., Vervink, K., Voong, D., Websdale, D., Wilkinson, G., Wotton, S. A., Wyllie, K., Xing, F., Young, R.
    Publicado 2013
    “…This provides charged particle identification over a wide momentum range, from 2–100 GeV/c. The operation and control, software, and online monitoring of the RICH system are described. …”
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    Online Artículo Texto
    Performance of the LHCb RICH detector at the LHC
  19. 20699
    “…At the NASA Space Radiation Laboratory (NSRL), we have proposed a GCR simulator, which implements a new rapid switching mode and higher energy beam extraction to 1.5 GeV/u, in order to integrate multiple ions into a single simulation within hours or longer for chronic exposures. …”
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    Online Artículo Texto
    Issues for Simulation of Galactic Cosmic Ray Exposures for Radiobiological Research at Ground-Based Accelerators
  20. 20700
    “…No instruments in the inner radiation belt are immune from the unforgiving penetration of the highly energetic protons (tens of MeV to GeV). The inner belt proton flux level, however, is relatively stable; thus, for any given instrument, the proton contamination often leads to a certain background noise. …”
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    Online Artículo Texto
    Upper limit on the inner radiation belt MeV electron intensity
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