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3601por Antinori, Federico, Bakke, H, Beusch, Werner, Bloodworth, Ian J, Caliandro, R, Carrer, N, Di Bari, D, Di Liberto, S, Elia, D, Evans, D, Fanebust, K, Fini, R A, Ftácnik, J, Ghidini, B, Grella, G, Helstrup, H, Holme, A K, Huss, D, Jacholkowski, A, Jones, G T, Kinson, J B, Knudson, K, Králik, I, Lenti, V, Lietava, R, Loconsole, R A, Løvhøiden, G, Manzari, V, Mazzoni, M A, Meddi, F, Michalon, A, Michalon-Mentzer, M E, Morando, M, Norman, P I, Pastircák, B, Quercigh, Emanuele, Romano, G, Safarík, K, Sándor, L, Segato, G F, Staroba, P, Thompson, M, Thorsteinsen, T F, Torrieri, G D, Tveter, T S, Urbán, J, Villalobos Baillie, O, Virgili, T, Votruba, M F, Závada, P“…A comprehensive study, including the most recent results, of yields and transverse mass spectra of K/sub S//sup 0/, Lambda , Xi /sup -/, Omega /sup -/ (and antiparticles) and negative particles as a function of the number of nucleons participating in the collisions is presented. (11 refs).…”
Publicado 2001
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3602por Miyazaki, K“…The derivative scalar coupling (DSC) model of relativistic nuclear matter by Zimanyi and Moszkowski is reconsidered from a constituent quark picture of nucleons. The DSC can be regarded as a correction to NNsigma coupling owing to the effect of scalar mean-field on the constituent quark. …”
Publicado 2003
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3603por Senger, P“…At beam energies where the number of produced particles is still small as compared to the number of participating nucleons, newly created particles can be used as probes for dense baryonic matter. …”
Publicado 2004
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3604“…Using extensive spectroscopic data on high spin states involving aligned valence nucleons in very neutron deficient nuclei above /sup 146/Gd the authors have derived the ground state masses of /sup 146 /Gd, /sup 147,148/Tb, /sup 148,149,150/Dy, /sup 149,150,151/Ho, and /sup 150,151,152/Er from a shell model analysis. …”
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3605“…From the perspective of microscopic approaches, the focus is on the direct resolution of the quantum A-body problem with a 2-body interaction between the nucleons as the only ingredient. In this contribution, we compare these two approaches for the first time by analyzing the differences in both formalism as well as by a comparison of the different valleys in the potential energy surfaces (PES), with a focus on the 240 Pu.…”
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3606por Andriamonje, S., Aune, S., Autiero, D., Barth, K., Belov, A., Beltran, B., Brauninger, H., Carmona, J.M., Cebrian, S., Collar, J.I., Dafni, T., Davenport, M., Di Lella, L., Eleftheriadis, C., Englhauser, J., Fanourakis, G., Ferrer-Ribas, E., Fischer, H., Franz, J., Friedrich, P., Geralis, T., Giomataris, I., Gninenko, S., Gomez, H., Hasinoff, M., Heinsius, F.H., Hoffmann, D.H.H., Irastorza, I.G., Jacoby, J., Jakovcic, K., Kang, D., Konigsmann, K., Kotthaus, R., Krcmar, M., Kousouris, K., Kuster, M., Lakic, B., Lasseur, C., Liolios, A., Ljubicic, A., Lutz, G., Luzon, G., Miller, D.W., Morales, J., Ortiz, A., Papaevangelou, T., Placci, A., Raffelt, G., Riege, H., Rodriguez, A., Ruz, J., Savvidis, I., Semertzidis, Y., Serpico, P., Stewart, L., Vieira, J.D., Villar, J., Vogel, J., Walckiers, L., Zioutas, K.“…This is the first such search for high-energy pseudoscalar bosons with couplings to nucleons conducted using a helioscope approach. No excess signal above background was found.…”
Publicado 2009
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3607“…Deep inelastic scattering of electrons and neutrinos on nucleons and electron–positron collisions have played a major role in this development. …”
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3608por Naskręt, Michał“…The mean number of wounded nucleons $\langle W\rangle$ extracted from the Glissando MC model is used to calculate the ratio $\langle \pi^- \rangle/\langle W\rangle.$ The results are compared to those from other experiments and their dependence on colliding systems and collision energy is discussed.…”
Publicado 2016
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3609por Aggarwal, M.M., Agnihotri, A., Ahammed, Z., Angelis, A.L.S., Antonenko, V., Arefiev, V., Astakhov, V., Avdeitchikov, V., Awes, T.C., Baba, P.V.K.S., Badyal, S.K., Baldine, A., Barabach, L., Barlag, C., Bathe, S., Batiounia, B., Bernier, T., Bhalla, K.B., Bhatia, V.S., Blume, C., Bock, R., Bohne, E.M., Borocz, Z., Bucher, D., Buijs, A., Busching, H., Carlen, L., Chalyshev, V., Chattopadhyay, S., Cherbatchev, R., Chujo, T., Claussen, A., Das, A.C., Decowski, M.P., Djordjadze, V., Donni, P., Doubovik, I., Dutt, S., Dutta Majumdar, M.R., El Chenawi, K., Eliseev, S., Enosawa, K., Foka, P., Fokin, S., Frolov, V., Ganti, M.S., Garpman, S., Gavrishchuk, O., Geurts, F.J.M., Ghosh, T.K., Glasow, R., Gupta, S.K., Guskov, B., Gustafsson, H.A., Gutbrod, H.H., Higuchi, R., Hrivnacova, I., Ippolitov, M., Kalechofsky, H., Kamermans, R., Kampert, K.H., Karadev, K., Karpio, K., Kato, S., Kees, S., Kim, H., Kolb, B.W., Kosarev, I., Koutcheryaev, I., Krumpel, T., Kugler, A., Kulinich, P., Kurata, M., Kurita, K., Kuzmin, N., Langbein, I., Lebedev, A., Lee, Y.Y., Lohner, H., Luquin, L., Mahapatra, D.P., Manko, V., Martin, M., Maximov, A., Mehdiyev, Rashid R., Mgebrichvili, G., Miake, Y., Mikhalev, D., Mir, M.F., Mishra, G.C., Miyamoto, Y., Morrison, Douglas R.O., Mukhopadhyay, D.S., Myalkovski, V., Naef, H., Nandi, B.K., Nayak, S.K., Nayak, T.K., Neumaier, S., Nianine, A., Nikitine, V., Nikolaev, S., Nilsson, P., Nishimura, S., Nomokonov, P., Nystrand, J., Obenshain, F.E., Oskarsson, A., Otterlund, I., Pachr, M., Parfenov, A., Pavliouk, S., Peitzmann, T., Petracek, V., Plasil, F., Pinanaud, W., Purschke, M.L., Raeven, B., Rak, J., Raniwala, R., Raniwala, S., Ramamurthy, V.S., Rao, N.K., Retiere, F., Reygers, K., Roland, G., Rosselet, L., Roufanov, I., Roy, C., Rubio, J.M., Sako, H., Sambyal, S.S., Santo, R., Sato, S., Schlagheck, H., Schmidt, H.R., Shabratova, G., Shah, T.H., Sibiriak, I., Siemiarczuk, T., Silvermyr, D., Sinha, B.C., Slavine, N., Soderstrom, K., Solomey, N., Sorensen, S.P., Stankus, P., Stefanek, G., Steinberg, P., Stenlund, E., Stuken, D., Sumbera, M., Svensson, T., Trivedi, M.D., Tsvetkov, A., Twenhofel, C., Tykarski, L., Urbahn, J., van Eijndhoven, N., van Nieuwenhuizen, G.J., Vinogradov, A., Viyogi, Y.P., Vodopianov, A.S., Voros, S., Wyslouch, B., Yagi, K., Yokota, Y., Young, G.R.“…A power law fit to the photon yield as a function of the number of participating nucleons gives a value of 1.12+or-0.03 for the exponent. …”
Publicado 1999
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3610por Antinori, Federico, Bakke, H, Beusch, Werner, Bloodworth, Ian J, Caliandro, R, Carrer, N, Di Bari, D, Di Liberto, S, Elia, D, Evans, D, Fanebust, K, Fini, R A, Ftácnik, J, Ghidini, B, Grella, G, Helstrup, H, Holme, A K, Huss, D, Jacholkowski, A, Jones, G T, Kinson, J B, Knudson, K P, Králik, I, Lenti, V, Lietava, R, Loconsole, R A, Løvhøiden, G, Manzari, V, Mazzoni, M A, Meddi, F, Michalon, A, Michalon-Mentzer, M E, Morando, M, Norman, P I, Pastircák, B, Quercigh, Emanuele, Romano, G, Safarík, K, Sándor, L, Segato, G F, Staroba, P, Thompson, M, Thorsteinsen, T F, Torrieri, G D, Tveter, T S, Urbán, J, Villalobos Baillie, O, Virgili, T, Votruba, M F, Závada, P“…Yields are studied as a function of the number of nucleons participating in the collision, NpartNpart, which is estimated using the Glauber model. …”
Publicado 1999
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3611por Pagano, Paolo“…In 2002, 2003, and 2004 it used a 160 GeV polarized muon beam coming from SPS and scattered off a $^{6}$LiD (deuteron) target. The nucleons in the target can be polarized either longitudinally or transversely with respect to the muon beam and 20% of the running time has been devoted to transverse polarization. …”
Publicado 2005
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3612por Bold, T“…In the sector of low transverse momenta, the main areas of interest are the charged particle multiplicities and their scaling with the number of participating nucleons. Studied in details are also the collective phenomena arising from the initial collision shape and maintained by the hydrodynamical system evolution from the initial hard scattered quarks and gluons to the hadronized particles. …”
Publicado 2014
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3613“…The restrictions of the structure of the weak neutral current imposed by single pion production cross sections on single nucleons are investigated. A general vector (V), axial-vector (A) neutral current with mod Delta I mod <or=1 is assumed, where the isovector V, A neutral currents are the neutral members of the isotriplets containing the charged weak currents. …”
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3614por Gaardhoje, J J“…It has now become possible to form reasonably large volumes (containing more than 300 nucleons) in central collisions between heavy ions, with energy and matter densities in some parts of the volume exceeding those expected for the phase transition from hadronic matter to deconfined quark and gluon matter. …”
Publicado 1997
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3615por Horn, I“…In 2002, 2003, and 2004 a 160 GeV/c polarised $\mu^{+}$ beam was utilized coming from SPS and scattered off a $^{6}$LiD (deuteron) target. The nucleons in the target can be polarised either longitudinally or transversely with respect to the $\mu^{+}$ beam. …”
Publicado 2005
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3616por Schmitt, L“…A polarised muon beam is used for deep inelastic scattering on a polarised target to study the spin structure of nucleons. The physics program connected to the hadron beams includes Primakoff scattering of pions and kaons to study their polarisabilities, central production of hybrids and glueballs in a proton beam on a liquid hydrogen target and production and leptonic and semi-leptonic decays of charmed hadrons. …”
Publicado 1999
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3617por Chomaz, P“…Atomic nuclei are made of nucleons, protons and neutrons, composed by quarks strongly interacting via gluons. …”
Publicado 2006
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3618“…However, a robust identification of suppression patterns as signatures of a deconfined QCD medium requires a detailed understanding of the "normal nuclear absorption" already present in proton-nucleus collisions, where the charmonium production cross sections increase less than linearly with the number of target nucleons. We analyse the J/$\psi$ production cross sections measured in proton-nucleus collisions in fixed target experiments, with proton beam energies from 200 to 920~GeV, and in d-Au collisions at RHIC, at $\sqrt{s_{_{NN}}}=200$~GeV, in the framework of the Glauber formalism, using several sets of parton distributions with and without nuclear modifications. …”
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3619“…In particular, we obtain a new size of the holographic baryon and find a precise form of the repulsive core of nucleons. This matrix model complements the instanton soliton picture of holographic baryons, whose small size turned out to be well below the natural length scale of the approximation involved there. …”
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3620por Höhne, Claudia“…The expectation is that in these large systems with about 360 participating nucleons such a transition is more likely because of a longer lifetime and higher energy density. …”
Publicado 2003
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