Materias dentro de su búsqueda.
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5601por Bagnaschi, E., Sakurai, K., Borsato, M., Buchmueller, O., Citron, M., Costa, J.C., De Roeck, A., Dolan, M.J., Ellis, J.R., Flächer, H., Heinemeyer, S., Lucio, M., Martínez Santos, D., Olive, K.A., Richards, A., Spanos, V.C., Suárez Fernández, I., Weiglein, G.“…We identify the mechanisms that operate in different regions of the pMSSM11 parameter space to bring the relic density of the lightest neutralino, $\tilde{\chi }^0_{1}$ , into the range indicated by cosmological data. In the fit including $(g-2)_\mu $ , coannihilations with $\tilde{\chi }^0_{2}$ and the Wino-like $\tilde{\chi }^\pm _{1}$ or with nearly-degenerate first- and second-generation sleptons are active, whereas coannihilations with the $\tilde{\chi }^0_{2}$ and the Higgsino-like $\tilde{\chi }^\pm _{1}$ or with first- and second-generation squarks may be important when the $(g-2)_\mu $ constraint is dropped. …”
Publicado 2017
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5602por Ruggles, Clive“…Thematic articles cover general themes such as cosmologies, calendars, navigation, orientations and alignments, and ancient perceptions of space and time. …”
Publicado 2015
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5603por Suchek, Stanislav“…Dark Matter composes a significant part of the observable Universe. Despite a solid cosmological evidence, its nature, properties and interaction with the Standard Model sector is still to be unraveled. …”
Publicado 2019
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5604“…We explain the origin of this discrepancy, discuss its implications for the HI power spectrum Fisher matrix forecasts and argue that it motivates the HI field-level cosmological inference. On small scales in redshift space we use the difference between the model and the truth as a proxy for the Fingers-of-God effect. …”
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5605por Nicolás, Bernal Hernández“…We discuss the constraints from collider searches and high-precision measurements, the cosmological constraints on the relic abundance of the neutralino candidate for the Dark Matter in the Universe and the gluino lifetime. …”
Publicado 2017
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5606por Ade, P.A.R., Aghanim, N., Armitage-Caplan, C., Arnaud, M., Ashdown, M., Atrio-Barandela, F., Aumont, J., Baccigalupi, C., Banday, A.J., Barreiro, R.B., Battaner, E., Benabed, K., Benoît, A., Benoit-Lévy, A., Bernard, J. -P., Bersanelli, M., Bertincourt, B., Bielewicz, P., Bobin, J., Bock, J.J., Bond, J.R., Borrill, J., Bouchet, F.R., Boulanger, F., Bridges, M., Bucher, M., Burigana, C., Cardoso, J. -F., Catalano, A., Challinor, A., Chamballu, A., Chary, R. -R., Chen, X., Chiang, L. -Y, Chiang, H.C., Christensen, P.R., Church, S., Clements, D.L., Colombi, S., Colombo, L.P.L., Combet, C., Couchot, F., Coulais, A., Crill, B.P., Curto, A., Cuttaia, F., Danese, L., Davies, R.D., de Bernardis, P., de Rosa, A., de Zotti, G., Delabrouille, J., Delouis, J. -M., Désert, F. -X., Dickinson, C., Diego, J.M., Dole, H., Donzelli, S., Doré, O., Douspis, M., Dupac, X., Efstathiou, G., Enßlin, T.A., Eriksen, H.K., Filliard, C., Finelli, F., Forni, O., Frailis, M., Franceschi, E., Galeotta, S., Ganga, K., Giard, M., Giardino, G., Giraud-Héraud, Y., González-Nuevo, J., Górski, K.M., Gratton, S., Gregorio, A., Gruppuso, A., Hansen, F.K., Hanson, D., Harrison, D., Helou, G., Henrot-Versillé, S., Hernández-Monteagudo, C., Herranz, D., Hildebrandt, S.R., Hivon, E., Hobson, M., Holmes, W.A., Hornstrup, A., Hovest, W., Huffenberger, K.M., Jaffe, T.R., Jaffe, A.H., Jones, W.C., Juvela, M., Keihänen, E., Keskitalo, R., Kisner, T.S., Kneissl, R., Knoche, J., Knox, L., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamarre, J. -M., Lasenby, A., Laureijs, R.J., Lawrence, C.R., Le Jeune, M., Lellouch, E., Leonardi, R., Leroy, C., Lesgourgues, J., Liguori, M., Lilje, P.B., Linden-Vørnle, M., López-Caniego, M., Lubin, P.M., Macías-Pérez, J.F., Maffei, B., Mandolesi, N., Maris, M., Marshall, D.J., Martin, P.G., Martínez-González, E., Masi, S., Matarrese, S., Matthai, F., Maurin, L., Mazzotta, P., McGehee, P., Meinhold, P.R., Melchiorri, A., Mendes, L., Mennella, A., Migliaccio, M., Mitra, S., Miville-Deschênes, M. -A., Moneti, A., Montier, L., Moreno, R., Morgante, G., Mortlock, D., Munshi, D., Murphy, J.A., Naselsky, P., Nati, F., Natoli, P., Netterfield, C.B., Nørgaard-Nielsen, H.U., Noviello, F., Novikov, D., Novikov, I., Osborne, S., Oxborrow, C.A., Paci, F., Pagano, L., Pajot, F., Paladini, R., Paoletti, D., Partridge, B., Pasian, F., Patanchon, G., Perdereau, O., Perotto, L., Perrotta, F., Piacentini, F., Piat, M., Pierpaoli, E., Pietrobon, D., Plaszczynski, S., Pointecouteau, E., Polenta, G., Ponthieu, N., Popa, L., Poutanen, T., Pratt, G.W., Prézeau, G., Prunet, S., Puget, J. -L., Rachen, J.P., Reinecke, M., Remazeilles, M., Renault, C., Ricciardi, S., Riller, T., Ristorcelli, I., Rocha, G., Rosset, C., Roudier, G., Rusholme, B., Santos, D., Savini, G., Shellard, E.P.S., Spencer, L.D., Starck, J. -L., Stolyarov, V., Stompor, R., Sudiwala, R., Sunyaev, R., Sureau, F., Sutton, D., Suur-Uski, A. -S., Sygnet, J. -F., Tauber, J.A., Tavagnacco, D., Techene, S., Terenzi, L., Tomasi, M., Tristram, M., Tucci, M., Umana, G., Valenziano, L., Valiviita, J., Van Tent, B., Vielva, P., Villa, F., Vittorio, N., Wade, L.A., Wandelt, B.D., Yvon, D., Zacchei, A., Zonca, A.“…The lower frequencies (below 353 GHz) are calibrated using the cosmological microwave background dipole.One of the components of this anisotropy results from the orbital motion of the satellite in the Solar System, and is therefore time-variable. …”
Publicado 2013
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5607por Buchmueller, O., Cavanaugh, R., Roeck, A. De, Dolan, M. J., Ellis, J. R., Flächer, H., Heinemeyer, S., Isidori, G., Marrouche, J., Santos, D. Martínez, Olive, K. A., Rogerson, S., Ronga, F. J., de Vries, K. J., Weiglein, G.“…We analyze the impact of data from the full Run 1 of the LHC at 7 and 8 TeV on the CMSSM with [Formula: see text] and [Formula: see text] and the NUHM1 with [Formula: see text] , incorporating the constraints imposed by other experiments such as precision electroweak measurements, flavour measurements, the cosmological density of cold dark matter and the direct search for the scattering of dark matter particles in the LUX experiment. …”
Publicado 2014
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5608por Bergano, Miguel, Rocha, Armando, Cupido, Luís, Barbosa, Domingos, Villela, Thyrso, Boas, José Vilas, Rocha, Graça, Smoot, George F.“…The detailed knowledge of the Milky Way radio emission is important to characterize galactic foregrounds masking extragalactic and cosmological signals. The update of the global sky models describing radio emissions over a very large spectral band requires high sensitivity experiments capable of observing large sky areas with long integration times. …”
Publicado 2016
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5609por Kruijssen, J. M. Diederik, Schruba, Andreas, Chevance, Mélanie, Longmore, Steven N., Hygate, Alexander P. S., Haydon, Daniel T., McLeod, Anna F., Dalcanton, Julianne J., Tacconi, Linda J., van Dishoeck, Ewine F.“…The physics of star formation and the deposition of mass, momentum, and energy into the interstellar medium by massive stars (‘feedback’) are the main uncertainties in modern cosmological simulations of galaxy formation and evolution1, 2. …”
Publicado 2019
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5610
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5611por Kozakai, Chihiro“…SUSY models which predict that the Lightest SUSY Particle (LSP) is the partner of the neutral W boson (wino) are especially attractive because they are compatible with the cosmological observations. Such models also predict that the second lightest SUSY particle is the charged wino whose mass is nearly degenerated to the neutral wino mass. …”
Publicado 2018
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5612por De Vries, Jacco Andreas“…This has lead to the ambition to explain large-scale cosmological observations starting from the very small scale of particle interactions. …”
Publicado 2018
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5613
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5614por Gonzalo, Eduardo“…The conjecture has far reaching consequences and applies to several interesting physical systems: i) Among chaotic inflation potentials only those asymptotically linear may survive. ii) If applied to the radion of the circle compactification of the Standard Model to 3D with Dirac neutrinos, the constraint implies that the 4D cosmological constant scale must be larger than the mass of the lightest neutrino, which must be in normal hierarchy. …”
Publicado 2019
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5615por Balbi, Amedeo“…Molte delle informazioni codificate nella radiazione cosmica di fondo sono state impresse dal sovrapporsi di onde acustiche presenti nell’Universo primordiale: una "musica" del Big Bang, che i cosmologi hanno tentato per anni di ricostruire, usando tecniche analoghe a quelle che permettono di distinguere il suono di diversi strumenti musicali. …”
Publicado 2007
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5616por Kirsanov, Mikhail“…The analysis of these data is not yet finished, although the sensitivity is already estimated as about 3 times better than in the previously published result on the 2016 data.For models considering scalar and fermionic thermal Dark Matter interacting with the visible sector through the vector portal the experiment starts to be sensitive to the regions of the dark-matter parameter predicted from the cosmological observations of Dark Matter.We also report the improved results on a direct search for a new 16.7 MeV boson (X) which could explain the anomalous excess of e+e- pairs observed in the excited 8Be* nucleus decays. …”
Publicado 2019
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5617por Genest, Marie-Helene“…Using WMAP (Wilkinson Microwave Anisotropy Probe) results on cosmic microwave background anisotropies, limits on the dark matter cosmological density can be set. These boundaries can then be converted in limits on the supersymmetric parameters, thus constraining the possible models of neutralino. …”
Publicado 2007
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5618por Irastorza, Igor G, Armengaud, E., Avignone, F. T., Betz, M., Brax, P., Brun, P., Cantatore, G., Carmona, J. M., Carosi, G. P., Caspers, F., Caspi, S., Cetin, S. A., Chelouche, D., Christensen, F. E., Dael, A., Dafni, T., Davenport, M., Derbin, A.V., Desch, K., Diago, A., Dobrich, B. D., Dratchnev, I., Dudarev, A., Eleftheriadis, C., Fanourakis, G., Ferrer-Ribas, E., Galan, J., Garcia, J. A., Garza, J. G., Geralis, T., Gimeno, B., Giomataris, I., Gninenko, S., Gomez, H., Gonzalez-Diaz, D., Guendelman, E., Hailey, C. J., Hiramatsu, T., Hoffmann, D. H. H., Horns, D., Iguaz, F. J., Isern, J., Imai, K., Jakobsen, A. C., Jaeckel, J., Jakovcic, K., Kaminski, J., Kawasaki, M., Karuza, M., Krcmar, M., Kousouris, K., Krieger, C., Lakic, B., Limousin, O., Lindner, A., Liolios, A., Luzon, G., Matsuki, S., Muratova, V. N., Nones, C., Ortega, I., Papaevangelou, T., Pivovaroff, M. J., Raffelt, G., Redondo, J., Ringwald, A., Russenschuck, S., Ruz, J., Saikawa, K., Savvidis, I., Sekiguchi, T., Semertzidis, Y. K., Shilon, I., Sikivie, P., Silva, H., Kate, H. ten, Tomas, A., Troitsky, S., Vafeiadis, T., van Bibber, K., Vedrine, P., Villar, J. A., Vogel, J. K., Walckiers, L., Weltman, A., Wester, W., Yildiz, S. C., Zioutas, K.“…At the very least it will firmly exclude a large region of this space of high cosmological and astrophysical relevance. In particular it will probe a large fraction of the high mass part (1 meV to 1 eV) of the QCD axion allowed window. …”
Publicado 2013
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5619por Colombo, Tommaso“…Nevertheless, the Standard Model is necessarily an incomplete theory as it does neither account for gravity, nor provide an explanation to cosmological problems like the apparent existence of dark matter and the observed matter-antimatter asymmetry. …”
Publicado 2013
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5620por Beauchemin , Pierre-Hugues“…However, given, for example, the Supersyminetric Large Extra Dimension (SLED) scenario, which can provide a framework for a solution to the cosmological constant problem, the D-dimensional Planck scale is approximately fixed and so is the graviton production rate. …”
Publicado 2017
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