12 results on '"statistical models (nuclear)"'
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Search Results
2. Neutral Kaon Interferometry in Au+Au collisions at sqrt(s_NN) = 200 GeV
- Author
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Abelev, B.I., Adams, J., Aggarwal, M.M., Ahammed, Z., Amonett, J., Anderson, B.D., Anderson, M., Arkhipkin, D., Averichev, G.S., Bai, Y., Balewski, J., Barannikova, O., Barnby, L.S., Baudot, J., Bekele, S., Belaga, V.V., Bellingeri-Laurikainen, A., Bellwied, R., Benedosso, F., Bhardwaj, S., Bhasin, A., Bhati, A.K., Bichsel, H., Bielcik, J., Bielcikova, J., Bland, L.C., Blyth, S.-L., Bonner, B.E., Botje, M., Bouchet, J., Brandin, A.V., Bravar, A., Bystersky, M., Cadman, R.V., Cai, X.Z., Caines, H., Calderon de la Barca Sanchez, M., Castillo, J., Catu, O., Cebra, D., Chajecki, Z., Chaloupka, P., Chattopadhyay, S., Chen, H.F., Chen, J.H., Cheng, J., Cherney, M., Chikanian, A., Christie, W., Coffin, J.P., Cormier, T.M., Cosentino, M.R., Cramer, J.G., Crawford, H.J., Das, D., Das, S., Daugherity, M., de Moura, M.M., Dedovich, T.G., DePhillips, M., Derevschikov, A.A., Didenko, L., Dietel, T., Djawotho, P., Dogra, S.M., Dong, W.J., Dong, X., Draper, J.E., Du, F., Dunin, V.B., Dunlop, J.C., Dutta Mazumdar, M.R., Eckardt, V., Edwards, W.R., Efimov, L.G., Emelianov, V., Engelage, J., Eppley, G., Erazmus, B., Estienne, M., Fachini, P., Fatemi, R., Fedorisin, J., Filimonov, K., Filip, P., Finch, E., Fine, V., Fisyak, Y., Fu, J., Gagliardi, C.A., Gaillard, L., Ganti, M.S., Ghazikhanian, V., Ghosh, P., Gonzalez, J.S., Gorbunov, Y.G., Gos, H., Grebenyuk, O., Grosnick, D., Guertin, S.M., Guimaraes, K.S.F.F., Guo, Y., Gupta, N., Gutierrez, T.D., Haag, B., Hallman, T.J., Hamed, A., Harris, J.W., He, W., Heinz, M., Henry, T.W., Hepplemann, S., Hippolyte, B., Hirsch, A., Hjort, E., Hoffman, A.M., Hoffmann, G.W., Horner, M.J., Huang, H.Z., Huang, S.L., Hughes, E.W., Humanic, T.J., Igo, G., Jacobs, P., Jacobs, W.W., Jakl, P., Jia, F., Jiang, H., Jones, P.G., Judd, E.G., Kabana, S., Kang, K., Kapitan, J., Kaplan, M., Keane, D., Kechechyan, A., Khodyrev, V.Yu., Kim, B.C., Kiryluk, J., Kisiel, A., Kislov, E.M., Klein, S.R., Kocoloski, A., Koetke, D.D., Kollegger, T., Kopytin, M., Kotchenda, L., Kouchpil, V., Kowalik, K.L., Kramer, M., Kravtsov, P., Kravtsov, V.I., Krueger, K., Kuhn, C., Kulikov, A.I., Kumar, A., Kuznetsov, A.A., Lamong, M.A.C., Landgraf, J.M., Lange, S., LaPointe, S., Laue, F., Lauret, J., Lebedev, A., Lednicky, R., Lee, C.-H., Lehocka, S., LeVine, M.J., Li, C., Li, Q., Li, Y., Lin, G., Lin, X., Lindenbaum, S.J., Lisa, M.A., Liu, f., Liu, H., Liu, J., Liu, L., Liu, Z., Ljubicic, T., Llope, W.J., Long, H., Longarche, R.S., Lopez-Noriega, M., Love, W.A., Lu, Y., Ludlam, T., Lynn, D., Ma, G.L., Ma, J.G., Ma, Y.G., Magestro, D., Mahapatra, D.P., Majka, R., Mangotra, L.K., Manweiler, R., Margetis, S., Markert, C., Martin, L., Matis, H.S., Matulenko, Yu.A., McClain, C.J., McShane, T.S., Melnick, Yu., Meschanin, A., Millane, J., Miller, M.L., Minaev, N.G., Mioduszewski, S., Mironov, C., Mischke, A., Mishra, D.K., Mitchell, J., Mohanty, B., Molnar, L., Moore, C.F., Morozov, D.A., Munhoz, M.G., Nandi, B.K., Nattrass, C., Nayak, T.K., Nelson, J.M., Netrakanti, P.K., Nikitin, V.A., Nogach, L.V., Nurushev, S.B., Odyniec, G., Ogawa, A., Okorokov, V., Oldenburg, M., Olson, D., Pachr, M., Pal, S.K., Panebratsev, Y., Panitkin, S.Y., Pavlinov, A.I., Pawlak, T., Peitzmann, T., Perevoztchikov, V., Perkins, C., Peryt, W., Petrov, V.A., Phatak, S.C., Picha, R., Planinic, M., Pluta, J., Poljak, N., Porile, N., Porter, J., Poskanzer, A.M., Potekhin, M., Potrebenikov, E., Potukuchi, B.V.K.S., Prindle, D., Pruneau, C., Putschke, J., Rakness, G., Raniwala, R., Raniwala, S., Ray, R.L., Razin, S.V., Reinnarth, J., Relyea, D., Retiere, F., Ridiger, A., Ritter, H.G., Roberts, J.B., Rogachevskiy, O.V., Romero, J.L., Rose, A., Roy, C., Ruan, L., Russcher, M.J., Sahoo, R., Sakuma, T., Salur, S., Sandweiss, J., Sarsour, M., Sazhin, P.S., Schambach, J., Scharenberg, R.P., Schmitz, N., Schweda, K., Seger, J., Selyuzhenkov, I., Seyboth, P., Shabetai, A., Shahaliev, E., Shao, M., Sharma, M., Shen, W.Q., Shimanskiy, S.S., Sichtermann, E., Simon, F., Singaraju, R.N., Smirnov, N., Snellings, R., Sood, G., Sorensen, P., Sowinski, J., Speltz, J., Spinka, H.M., Srivastava, B., Stadnik, A., Stanislaus, T.D.S., Stock, R., Stolpovsky, A., Strikhanov, M., Stringfellow, B., Suaide, A.A.P., Sugarbaker, E., Sumbera, M., Sun, Z., Surrow, B., Swager, M., Symons, T.J.M., Szanto de Toledo, A., Tai, A., Takahaski, J., Tang, A.H., Tarnowsky, T., Thein, D., Thomas, J.H., Timmins, A.R., Timoshenko, S., Tokarev, M., Trainor, T.A., Trentalange, S., Tribble, R.E., Tsai, O.D., Ulery, J., Ullrich, T., Underwood, D.G., Van Buren, G., van der Kolk, N., van Leeuwen, M., Vander Molen, A.M., Varma, R., Vasilevski, I.M., Vasiliev, A.N., Vernet, R., Vigdor, S.E., Viyogi, Y.P., Vokal, S., Voloshin, S.A., Waggoner, W.T., Wang, F., Wang, G., Wang, J.S., Wang, X.L., Wang, Y., Watson, J.W., Webb, J.C., Westfall, G.D., Wetzler, A., Whitten Jr., C., Wieman, H., Wissink, S.W., Witt, R., Wood, J., Wu, J., Xu, N., Xu, Q.L., Xu, Z., Yepes, P., Yoo, I.-K., Yurevich, V.I., Zhan, W., Zhang, H., Zhang, W.M., Zhang, Y., Zhang, Z.P., Zhao, Y., Zhong, C., Zoulkarneev, R., Zoulkarneeva, Y., Zubarev, A.N., Zuo, J.X., Département Recherches Subatomiques (DRS-IPHC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Louis Pasteur - Strasbourg I-Centre National de la Recherche Scientifique (CNRS), Laboratoire SUBATECH Nantes (SUBATECH), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Nantes (UN)-Mines Nantes (Mines Nantes), STAR, and Mines Nantes (Mines Nantes)-Université de Nantes (UN)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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quark-gluon plasma ,Physics ,statistical models (nuclear) ,FOS: Physical sciences ,nuclei with mass number 190 to 219 ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,25.75.Gz ,heavy ion-nucleus reactions ,High Energy Physics::Experiment ,Astrophysics::Earth and Planetary Astrophysics ,Nuclear Experiment (nucl-ex) ,kaon production ,Nuclear Experiment - Abstract
We present the first statistically meaningful results from two-K0s interferometry in heavy-ion collisions. A model that takes the effect of the strong interaction into account has been used to fit the measured correlation function. The effects of single and coupled channel were explored. At the mean transverse mass m_T = 1.07 GeV, we obtain the values R = 4.09 +/- 0.46 (stat.) +/- 0.31 (sys) fm and lambda = 0.92 +/- 0.23 (stat) +/- 0.13 (sys), where R and lambda are the invariant radius and chaoticity parameters respectively. The results are qualitatively consistent with m_T systematics established with pions in a scenario characterized by a strong collective flow., Comment: 11 pages, 10 figures
- Published
- 2008
3. Fast Decision in Favor of the Slow Fission Process
- Author
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A. Letourneau, C.-M. Herbach, J. Galin, V. Tishchenko, Frank Goldenbaum, D. Hilscher, W. U. Schröder, U. Jahnke, Grand Accélérateur National d'Ions Lourds (GANIL), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,Fissility ,24.75.+i, 24.10.-i, 25.40.Sc, 24.60.Dr ,Photon ,Fission ,Nuclear Theory ,statistical models (nuclear) ,General Physics and Astronomy ,Alpha particle ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Approx ,proton-nucleus reactions ,Excited state ,ddc:550 ,fission ,Multiplicity (chemistry) ,Atomic physics ,Nuclear Experiment ,Excitation - Abstract
The fission probability P{sub f} of highly excited targetlike nuclei produced in reactions of 2.5 GeV protons on Au, Bi, and U was studied as a function of excitation energy E* whereby E* is deduced eventwise from the multiplicity of evaporated light particles. At the highest E* of 1000 MeV P{sub f} amounts to {approx_equal}30% with all 3 target nuclei irrespective of the initial fissility. Statistical-model calculations satisfactorily reproduce the observed evolution of P{sub f} with E* - provided that no extra transient delay is introduced. Fission thus is decided upon very fast and early in the long deexcitation chain towards scission which comprises as much as {approx_equal}80% of all evaporated alpha particles.
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- 2005
4. Statistical Approaches to the Even-odd Effect in Fission
- Author
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F. Rejmund, A. Kelic, A.V. Ignatyuk, Kjeld Schmidt, M. V. Ricciardi, Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), H. Goutte, H. Faust, G. Fioni, and D. Goutte
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Nuclear physics ,Fission ,Scientific method ,statistical models (nuclear) ,fission ,Nuclide ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Biology ,nuclear charge ,25.85.-w, 24.10.Pa, 21.10.Ft ,Effective nuclear charge - Abstract
Statistical approaches have been widely used for describing the nuclear-fission process. They were quite successful in explaining several prominent features of the global nuclide distributions and many other aspects, while there are controversial conclusions on the origin of the even-odd effect in the nuclear-charge yields. We analyze the ingredients of the main statistical approaches to the even-odd effect in fission and show up that many of their deficiencies rely on unrealistic assumptions. Finally, we demonstrate that the large body of experimental results, obtained in the recent years to a great part at GSI, Darmstadt, is very successfully reproduced by a new stringent statistical approach.
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- 2005
5. Density of states in multifragmentation obtained using the Laplace transform method
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A. J. Cole, Laboratoire de Physique Subatomique et de Cosmologie (LPSC), and Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS)
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Canonical ensemble ,Statistical ensemble ,Physics ,Nuclear and High Energy Physics ,Partition function (statistical mechanics) ,Laplace transform ,[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th] ,010308 nuclear & particles physics ,statistical models (nuclear) ,Laplace transforms ,nuclear density ,Statistical mechanics ,nuclear fragmentation ,Statistical weight ,nuclear charge ,01 natural sciences ,Microcanonical ensemble ,nuclear mass ,25.70.Pq, 25.70.Mn, 24.60.Ky ,0103 physical sciences ,Density of states ,Statistical physics ,010306 general physics - Abstract
In equilibrium statistical mechanics, the density of microstates representing the statistical weight associated with a partition of an isolated system into subsystems (fragments) is the convolution of the state densities of the component subsystems. The Laplace transform approximation provides a simple representation of this density. Despite the fact that no external heat bath can be said to exist (the canonical ensemble is not appropriate) the approximation leads to partition probabilities that involve a product of factors (one for each fragment) expressed in terms of a characteristic inverse temperature. We apply the method to nuclear multifragmentation with particular emphasis on a transition that occurs when the major part of the available energy appears as kinetic (as opposed to internal excitation) energy of fragments. Finally, we discuss the shortcomings and advantages of expressing the weights of partitions with fixed total mass (charge) and multiplicity in a simple multinomial form.
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- 2005
6. Spectral statistics of Hamiltonian matrices in tridiagonal form
- Author
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J. Retamosa, Rafael A. Molina, Armando Relaño, A. P. Zuker, Institut de Recherches Subatomiques (IReS), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Cancéropôle du Grand Est-Université Louis Pasteur - Strasbourg I-Centre National de la Recherche Scientifique (CNRS)
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Physics ,Nuclear and High Energy Physics ,Band matrix ,Tridiagonal matrix ,[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th] ,010308 nuclear & particles physics ,Mathematical analysis ,Termodinámica ,statistical models (nuclear) ,Tridiagonal matrix algorithm ,Block matrix ,matrix algebra ,01 natural sciences ,Matrix (mathematics) ,Lanczos resampling ,21.10.Dr, 05.45.Mt, 24.60.Lz ,Matrix splitting ,Quantum mechanics ,0103 physical sciences ,010306 general physics ,Random matrix - Abstract
When a matrix is reduced to Lanczos tridiagonal form, its matrix elements can be divided into an analytic smooth mean value and a fluctuating part. The next-neighbor spacing distribution P(s) and the spectral rigidity $\Delta_3$ are shown to be universal functions of the average value of the fluctuating part. It is explained why the behavior of these quantities suggested by random matrix theory is valid in far more general cases.
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- 2005
7. Damping mechanisms and order-to-chaos transition in the warm rotating $^{163}$Er nucleus
- Author
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Leoni, S., Benzoni, G., Bracco, A., Blasi, N., Camera, F., Grassi, C., Mason, P., Million, B., Paleni, A., Pignanelli, M., Vigezzi, E., Wieland, O., Matsuo, M., Døssing, T., Herskind, B., B. Hagemann, G., Wilson, J., Maj, A., Kmiecik, M., Lo Bianco, G., M. Petrache, C., Castoldi, M., Zucchiatti, A., De Angelis, G., R. Napoli, D., Bednarczyk, P., Curien, D., Institut de Recherches Subatomiques (IReS), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Cancéropôle du Grand Est-Université Louis Pasteur - Strasbourg I-Centre National de la Recherche Scientifique (CNRS)
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nuclear spin ,yrast states ,nuclear shell model ,nuclear energy level transitions ,21.10.Re, 21.60.Ka, 23.20.Lv, 27.70.+q ,statistical models (nuclear) ,nuclei with mass number 150 to 189 ,gamma-ray spectra ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,nuclear cranking model ,nuclear rotational states - Abstract
The $\gamma$ decay in the quasicontinuum is used to study the order-to-chaos transition in the thermally excited $^{163}$Er nucleus. The experimental analysis is performed on high-statistics EUROBALL data, focusing on the spin region I$\approx (20–40) \hbar$, and internal excitation energy up of $\approx$ 2.5 MeV. The results are compared to cranked shell model calculations for this nucleus, taking into account the dependence on the K quantum number. Two main topics are investigated. First, the validity of the selection rules associated with the K quantum number are studied as a function of the internal energy U above yrast. K-selection rules are found to be obeyed in the decay along discrete unresolved rotational bands up to U $\approx$ 1.2 MeV, whereas in the interval U $\approx$ 1.2–2.5 MeV, where the order-to-chaos transition is expected to take place, selection rules are found to be only partially valid. Second, the line-shape analysis of $\gamma-\gamma$ coincidence spectra provides a direct experimental measurement of the rotational and compound damping widths ($\Gamma_{rot}$ and $\Gamma\mu$), yielding values of 200 and 20 keV, respectively, in good agreement with theory.
- Published
- 2005
8. Measurement of Nonrandom Event-by-Event Fluctuations of Average Transverse Momentum in $\sqrt{s_{NN}}$=200 GeV Au+Au and p+p Collisions
- Author
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Adler, S.S., Afanasiev, S., Aidala, C., Ajitanand, N.N., Akiba, Y., Alexander, J., Amirikas, R., Aphecetche, Laurent, Aronson, S.H., Averbeck, R., Awes, T.C., Azmoun, R., Babintsev, V., Baldisseri, A., Barish, K.N., Barnes, P.D., Bassalleck, B., Bathe, S., Batsouli, S., Baublis, V., Bazilevsky, A., Belikov, S., Berdnikov, Y., Bhagavatula, S., Boissevain, J.G., Borel, H., Borenstein, S., Brooks, M.L., Brown, D.S., Bruner, N., Bucher, D., Buesching, H., Bumazhnov, V., Bunce, G., Burward-Hoy, J.M., Butsyk, S., Camard, X., Chai, J.-S., Chand, P., Chang, W.C., Chernichenko, S., Chi, C.Y., Chiba, J., Chiu, M., Choi, I.J., Choi, J., Choudhury, R.K., Chujo, T., Cianciolo, V., Cobigo, Y., Cole, B.A., Constantin, P., D'Enterria, D.G., David, G., Delagrange, H., Denisov, A., Deshpande, A., Desmond, E.J., Dietzsch, O., Drapier, O., Drees, A., Du Rietz, R., Durum, A., Dutta, D., Efremenko, Y.V., El Chenawi, K., Enokizono, A., En'Yo, H., Esumi, S., Ewell, L., Fields, D.E., Fleuret, F., Fokin, S.L., Fox, B.D., Fraenkel, Z., Frantz, J.E., Franz, A., Frawley, A.D., Fung, S.-Y., Garpman, S., Ghosh, T.K., Glenn, A., Gogiberidze, G., Gonin, M., Gosset, J., Goto, Y., Granier De Cassagnac, R., Grau, N., Greene, S.V., Grosse Perdekamp, M., Guryn, W., Gustafsson, H.-Å., Hachiya, T., Haggerty, J.S., Hamagaki, H., Hansen, A.G., Hartouni, E.P., Harvey, M., Hayano, R., He, X., Heffner, M., Hemmick, T.K., Heuser, J.M., Hibino, M., Hill, J.C., Holzmann, W., Homma, K., Hong, B., Hoover, A., Ichihara, T., Ikonnikov, V.V., Imai, K., Isenhower, D., Ishihara, M., Issah, M., Isupov, A., Jacak, B.V., Jang, W.Y., Jeong, Y., Jia, J., Jinnouchi, O., Johnson, B.M., Johnson, S.C., Joo, K.S., Jouan, D., Kametani, S., Kamihara, N., Kang, J.H., Kapoor, S.S., Katou, K., Kelly, Steven, Khachaturov, B., Khanzadeev, A., Kikuchi, J., Kim, D.H., Kim, D.J., Kim, D.W., Kim, E., Kim, G.-B., Kim, H.J., Kistenev, E., Kiyomichi, A., Kiyoyama, K., Klein-Boesing, C., Kobayashi, H., Kochenda, L., Kochetkov, V., Koehler, D., Kohama, T., Kopytine, M., Kotchetkov, D., Kozlov, A., Kroon, P.J., Kuberg, C.H., Kurita, K., Kuroki, Y., Kweon, M.J., Kwon, Y., Kyle, G.S., Lacey, R., Ladygin, V., Lajoie, J.G., Lebedev, A., Leckey, S., Lee, D.M., Lee, S., Leitch, M.J., Li, X.H., Lim, H., Litvinenko, A., X. Liu, M., Liu, Yehan, Maguire, C.F., Makdisi, Y.I., Malakhov, A., Manko, V.I., Mao, Y., Martinez Garcia, Gines, Marx, M.D., Masui, H., Matathias, F., Matsumoto, T., McGaughey, P.L., Melnikov, E., Messer, F., Miake, Y., Milan, J., Miller, T.E., Milov, A., Mioduszewski, S., Mischke, R.E., Mishra, G.C., Mitchell, J.T., Mohanty, A.K., Morrison, D.P., Moss, J.M., Mühlbacher, F., Mukhopadhyay, D., Muniruzzaman, M., Murata, J., Nagamiya, S., Nagle, J.L., Nakamura, T., Nandi, B.K., Nara, M., Newby, J., Nilsson, P., Nyanin, A.S., Nystrand, J., O'Brien, E., Ogilvie, C.A., Ohnishi, H., Ojha, I.D., Okada, K., Ono, M., Onuchin, V., Oskarsson, A., Otterlund, I., Oyama, K., Ozawa, K., Pal, D., Palounek, A.P.T., Pantuev, V.S., Papavassiliou, V., Park, J., Parmar, A., Pate, S.F., Peitzmann, T., Peng, J.-C., Peresedov, V., Pinkenburg, C., P. Pisani, R., Plasil, F., Purschke, M.L., Purwar, A.K., Rak, J., Ravinovich, I., Read, K.F., Reuter, M., Reygers, K., Riabov, V., Riabov, Y., Roche, G., Romana, A., Rosati, M., Rosnet, P., Ryu, S.S., Sadler, M.E., Saito, N., Sakaguchi, T., Sakai, M., Sakai, S., Samsonov, V., Sanfratello, L., Santo, R., Sato, H.D., Sato, S., Sawada, S., Schutz, Y., Semenov, V., Seto, R., Shaw, M.R., Shea, T.K., Shibata, T.-A., Shigaki, K., Shiina, T., Silva, C.L., Silvermyr, D., Sim, K.S., P. Singh, C., Singh, V., Sivertz, M., Soldatov, A., Soltz, R.A., Sondheim, W.E., Sorensen, S.P., V. Sourikova, I., Staley, F., Stankus, P.W., Stenlund, E., Stepanov, M., Ster, A., P. Stoll, S., Sugitate, T., Sullivan, J.P., Takagui, E.M., Taketani, A., Tamai, M., Tanaka, K.H., Tanaka, Y., Tanida, K., Tannenbaum, M.J., Tarján, P., Tepe, J.D., Thomas, T.L., Tojo, J., Torii, H., Towell, R.S., Tserruya, I., Tsuruoka, H., Tuli, S.K., Tydesjö, H., Tyurin, N., Van Hecke, H.W., Velkovska, J., Velkovsky, M., Villatte, L., Vinogradov, A.A., Volkov, M.A., Vznuzdaev, E., Wang, X.R., Watanabe, Y., White, S.N., Wohn, F.K., Woody, C.L., Xie, W., Yang, Y., Yanovich, A., Yokkaichi, S., Young, G.R., Yushmanov, I.E., Zajc, W.A., Zhang, C., Zhou, S., Zhou, S.J., Zolin, L., Laboratoire SUBATECH Nantes (SUBATECH), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Nantes (UN)-Mines Nantes (Mines Nantes), Laboratoire Leprince-Ringuet (LLR), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Laboratoire de Physique Corpusculaire - Clermont-Ferrand (LPC), Université Blaise Pascal - Clermont-Ferrand 2 (UBP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), PHENIX, Mines Nantes (Mines Nantes)-Université de Nantes (UN)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), and Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
- Subjects
statistical models (elementary particles) ,proton-proton inclusive interactions ,25.75.Dw ,statistical models (nuclear) ,[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] ,heavy ion-nucleus reactions ,nuclei with mass number 190 to 219 ,hard collision models ,Nuclear Experiment - Abstract
EI; Event-by-event fluctuations of the average transverse momentum of produced particles near midrapidity have been measured by the PHENIX Collaboration in sqrt(s[sub NN])=200 GeV Au+Au, and p+p collisions at the Relativistic Heavy Ion Collider. The fluctuations are observed to be in excess of the expectation for statistically independent particle emission for all centralities. The excess fluctuations exhibit a dependence on both the centrality of the collision and on the pT range over which the average is calculated. Both the centrality and pT dependence can be well reproduced by a simulation of random particle production with the addition of contributions from hard-scattering processes.
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- 2004
9. Analytical treatment of constraints in fragmentation
- Author
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A. J. Cole, Laboratoire de Physique Subatomique et de Cosmologie (LPSC), and Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,Nuclear and High Energy Physics ,Mathematical optimization ,010308 nuclear & particles physics ,probability ,Fragmentation (computing) ,statistical models (nuclear) ,nuclear fragmentation ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,25.70.Pq, 25.70.Mn, 24.60.Ky ,0103 physical sciences ,Poisson distribution ,010306 general physics ,Nuclear Experiment - Abstract
In fragmentation of a finite object such as an atomic nucleus or a percolation lattice, the multidimensional probability distribution of the numbers of fragments of each mass (charge, size) may be approximated as a product of Poisson distributions. In this work we present an analytical treatment of the influence of constraints (multiplicity, mass, etc.) that may be imposed on the basic product distribution.
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- 2004
10. Characteristics of the fragments produced in central collisions of 129Xe+ natSn from 32 to 50 AMeV
- Author
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Hudan, S., Chbihi, A., Frankland, J.D., Mignon, A., Wieleczko, J.P., Auger, G., Bellaize, N., Borderie, B., Botvina, A., Bougault, R., Bouriquet, B., Buta, A., Colin, J., Cussol, D., Dayras, R., Durand, D., Galichet, E., Guinet, D., Guiot, B., Lanzalone, G., Lautesse, P., Lavaud, F., Lecolley, J.F., Legrain, R., Le Neindre, N., Lopez, O., Manduci, L., Marie, J., Nalpas, L., Normand, J., Pârlog, M., Pawlowski, P., Picheon, M., Plagnol, E., Rivet, M.F., Rosato, E., Roy, R., Steckmeyer, J.C., Tabacaru, G., Tamain, B., Van Lauwe, A., Vient, E., Vigilante, M., Volant, C., Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), INDRA, Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
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nuclei with mass number 90 to 149 ,25.70.Pq ,statistical models (nuclear) ,heavy ion-nucleus reactions ,FOS: Physical sciences ,nuclear fragmentation ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Nuclear Experiment (nucl-ex) ,Nuclear Experiment - Abstract
Characteristics of the primary fragments produced in central collisions of 129Xe + natSn from 32 to 50 AMeV have been obtained. By using the correlation technique for the relative velocity between light charged particles (LCP) and fragments, we were able to extract the multiplicities and average kinetic energy of secondary evaporated LCP. We then reconstructed the size and excitation energy of the primary fragments. For each bombarding energy a constant value of the excitation energy per nucleon over the whole range of fragment charge has been found. This value saturates at 3 AMeV for beam energies 39 AMeV and above. The corresponding secondary evaporated LCP represent less than 40% of all produced particles and decreases down to 23% for 50 AMeV. The experimental characteristics of the primary fragments are compared to the predictions of statistical multifragmentation model (SMM) calculations. Reasonable agreement between the data and the calculation has been found for any given incident energy. However SMM fails to reproduce the trend of the excitation function of the primary fragment excitation energy and the amount of secondary evaporated LCP's., Comment: 14 pages, 17 included figures; typeset using ReVTeX4; submitted to Phys. Rev. C
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- 2002
- Full Text
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11. Measurement of Nonrandom Event-by-Event Fluctuations of Average Transverse Momentum in √sNN = 200 GeV Au + Au and p + p Collisions
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PHENIX Collaboration, Enokizono, Akitomo, Hachiya, Takashi, Homma, Kensuke, Kohama, Takeshi, Nakamura, Tomoaki, Shigaki, Kenta, Sugitate, Toru, PHENIX Collaboration, Enokizono, Akitomo, Hachiya, Takashi, Homma, Kensuke, Kohama, Takeshi, Nakamura, Tomoaki, Shigaki, Kenta, and Sugitate, Toru
- Abstract
type:text, Event-by-event fluctuations of the average transverse momentum of produced particles near midrapidity have been measured by the PHENIX Collaboration in √sNN = 200 GeV Au + Au, and p + p collisions at the Relativistic Heavy Ion Collider. The fluctuations are observed to be in excess of the expectation for statistically independent particle emission for all centralities. The excess fluctuations exhibit a dependence on both the centrality of the collision and on the pT range over which the average is calculated. Both the centrality and pT dependence can be well reproduced by a simulation of random particle production with the addition of contributions from hard-scattering processes.
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- 2004
12. Measurement of Nonrandom Event-by-Event Fluctuations of Average Transverse Momentum in √sNN = 200 GeV Au + Au and p + p Collisions
- Author
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PHENIX Collaboration, Enokizono, Akitomo, Hachiya, Takashi, Homma, Kensuke, Kohama, Takeshi, Nakamura, Tomoaki, Shigaki, Kenta, Sugitate, Toru, PHENIX Collaboration, Enokizono, Akitomo, Hachiya, Takashi, Homma, Kensuke, Kohama, Takeshi, Nakamura, Tomoaki, Shigaki, Kenta, and Sugitate, Toru
- Abstract
Event-by-event fluctuations of the average transverse momentum of produced particles near midrapidity have been measured by the PHENIX Collaboration in √sNN = 200 GeV Au + Au, and p + p collisions at the Relativistic Heavy Ion Collider. The fluctuations are observed to be in excess of the expectation for statistically independent particle emission for all centralities. The excess fluctuations exhibit a dependence on both the centrality of the collision and on the pT range over which the average is calculated. Both the centrality and pT dependence can be well reproduced by a simulation of random particle production with the addition of contributions from hard-scattering processes.
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