NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = I.Sedykh Found 28 matches. 2022DA01 Phys.Rev. C 105, 014620 (2022) O.I.Davydovska, V.Yu.Denisov, I.Yu.Sedykh Evaluation of the fission barrier values using the experimental values of the ratio Γf(E)/Γn(E) NUCLEAR STRUCTURE 180,181,182,184W, 185Re, 186,187,188,190Os, 189,191Ir, 192,193,194,196Pt, 195,197Au, 196,198,199,200Hg, 201Tl, 207,209Bi, 208,210,211,212Po, 213At; analyzed experimental data for ratios of fission widths Γf and neutron evaporation width Γn as function of thermal excitation energies of the compound nuclei using statistical approach for fission barrier heights. Comparison with the results of the macroscopic-microscopic finite-range liquid-drop model.
doi: 10.1103/PhysRevC.105.014620
2022DE01 Phys.Lett. B 824, 136814 (2022) Dependence of average total kinetic energy of fission fragments on excitation energy of fissioning nucleus NUCLEAR REACTIONS 233,235,238U, 239Pu(n, F), E<100 MeV; analyzed available data. 234,236,239U, 240Pu; deduced average total kinetic energy of fission fragments using statistical model.
doi: 10.1016/j.physletb.2021.136814
2022DE02 Phys.Rev. C 105, 014616 (2022) Dependence of average total kinetic energy of fission fragments on the excitation energy of the compound nucleus NUCLEAR REACTIONS 233,235,238U, 239Pu(n, F), E=thermal; analyzed experimental data for average total kinetic energy (TKE) release of fission fragments on the excitation energy of 10-100 MeV for 234,236U, <500 MeV for 239U, and <300 MeV for 240Pu compound nuclei using a simple statistical model. Discussed origin of the energy dependence of the average total kinetic energy in neutron-induced fission.
doi: 10.1103/PhysRevC.105.014616
2021DE10 Eur.Phys.J. A 57, 129 (2021) Calculation of fission fragment characteristics for the reactions nth + 235U and n14MeV+235U NUCLEAR REACTIONS 235U(n, F), E thermal; 235U(n, F), E=14 MeV; calculated potential energy surfaces, radial dependence of α-nucleus potential, mass distributions of fission fragments using 3+4 and 4 body, the deformation energy and the ground-state deformation of fragments in the Strutinsky shell correction approach with the Cherpurnov parametrization of the Woods-Saxon potential. Comparison with experimental data.
doi: 10.1140/epja/s10050-021-00433-8
2021DE15 Chin.Phys.C 45, 044106 (2021) Production of super-heavy nuclei in cold fusion reactions NUCLEAR REACTIONS 208Pb(50Ti, X), (52Cr, X), (54Cr, X), (58Fe, X), (64Ni, X), (70Zn, X), (78Ge, X), E not given; calculated potential energy landscape as a function of the Z and deformation parameter.
doi: 10.1088/1674-1137/abdfc0
2019DE01 Chin.Phys.C 43, 014101 (2019) V.Yu.Denisov, O.A.Belyanovska, V.P.Khomenkov, I.Yu.Sedykh, K.M.Sukhyy A simple description of the temperature dependence of the width of the fission-fragment mass yield in 197Au and 209Bi at intermediate energies NUCLEAR REACTIONS 197Au, 209Bi(γ, F), E=460-896 MeV; calculated the temperature dependence of the fission-fragment widths. Comparison with experimental data.
doi: 10.1088/1674-1137/43/1/014101
2019DE26 Eur.Phys.J. A 55, 153 (2019) Empirical relations for the fusion cross sections of heavy ions NUCLEAR REACTIONS 12C(12C, x) to 124Sn(58Ni, x); compiled experimental σ for 85 even-even heavy-ion systems; calculated barrier height B, radius R, curvature hω using Wong formula; deduced formula parameters using fit to the data; calculated, estimated fusion σ, astrophysical S-factor, calculated surface deformation parameter of multipole vibrations of projectile and target nuclei, Q-values of K-neutron pickup or stripping processes, fusion σ for 85 reactions and E=2-164 MeV; 12,14,18C(12C, x), (14C, x)(18C, x), E=2-5.8 MeV; calculated astrophysical S-factor.
doi: 10.1140/epja/i2019-12855-6
2018DE28 Phys.Rev. C 98, 024601 (2018) Calculation of the fission width of an excited nucleus with the fission barrier dependent on excitation energy NUCLEAR STRUCTURE 238Pu, 286Cn; calculated excitation energy dependent fission barrier with pairing, shell correction, and liquid-drop contributions, ratio of fission widths and Bohr-Wheeler fission widths of excited compound nuclei using Strutinsky shell correction prescription and the liquid-drop model.
doi: 10.1103/PhysRevC.98.024601
2018DE41 Eur.Phys.J. A 54, 231 (2018) Calculation of the ratio Γn(E)/Γf(E) in various approaches for the fission width NUCLEAR STRUCTURE 188Os, 210,212Po; calculated excited nuclei width for the neutron emission Γn(E) and that for fission Γf(E) vs E* using the Bohr-Wheeler approach (and also some other methods). Compared with available data.
doi: 10.1140/epja/i2018-12660-9
2017DE01 Nucl.Phys. A958, 101 (2017) V.Yu.Denisov, T.O.Margitych, I.Yu.Sedykh Mass yields and kinetic energy of fragments from fission of highly-excited nuclei with A≤220 NUCLEAR STRUCTURE A≤220; calculated quadrupole, octupole, hexadecapole fragment deformation, Q vs mass number. NUCLEAR REACTIONS 142Nd(40Ca, F), E not given;144Sm(36Ar, F), E not given;182W(13C, F), E not given;184W(34S, F), E not given;186W(24Mg, F), E not given;194Pt(16O, F), E not given;197Au(α, F), E not given;208Pb(19F, F), E not given; calculated fission yields vs fragment mass using trajectory concept.
doi: 10.1016/j.nuclphysa.2016.11.007
2017DE04 Phys.Rev. C 95, 014605 (2017) V.Yu.Denisov, N.A.Pilipenko, I.Yu.Sedykh Interaction of three fission fragments and yields of various ternary fragments RADIOACTIVITY 252Cf(SF); calculated differences of the potentials for deformation parameters at the lowest barrier point for fission into 98Zr+22O+132Sn and 72Ni+48Ca+132Sn, dependence of total excitation energy of fragments for the triple spontaneous fission on the masses of the first and third, and first and second fragments, also at an excitation energy of 10 MeV. 250Cf(SF); calculated yield of probability per binary fission event of ternary particles, and compared with experimental data. Simple macroscopic model, with three collinear touching deformed fission fragments formed during the three-fragment fission after scission of necks.
doi: 10.1103/PhysRevC.95.014605
2017DE14 Nucl.Phys. A963, 15 (2017) Fission-fragment mass yields of highly excited nuclei with 119 ≤ A ≤ 218 produced in various reactions NUCLEAR REACTIONS 197Au, 209Bi(γ, f), E=1000 MeV[from bremsstrahlung, stated γ energy is the end-point energy];139La, 165Ho, 197Au(α, f), E not given; calculated fission mass yields. 99Ru(20Ne, f), E=124 MeV;112Sn(12C, f), E=137 MeV;124Sn(20Ne, f), E=140 MeV;154Sm(35Cl, f), E=163.7 MeV;176Yb(28Si, f), E=189 MeV;181Ta(19F, f), E not given;184W(16O, f), E not given;184W28Si, f), E=166, 189 MeV;186W(20Ne, f), E=142, 174 MeV;198Pt, 197Au, 206Pb(12C, f), E not given;197Au(16O, f), E not given; calculated mass yield (in the case of 16O+184W also the charge distribution employing number of states of two-fragment systems at the saddle point. Compared with published data.
doi: 10.1016/j.nuclphysa.2017.04.002
2015DE20 Phys.Rev. C 92, 014602 (2015) V.Yu.Denisov, O.I.Davidovskaya, I.Yu.Sedykh Improved parametrization of the unified model for α decay and α capture RADIOACTIVITY A=105-115(α); A=150-260(α); analyzed known ground-state-to-ground-state α-transition half-lives for 401 nuclides and determined parameters in the framework of unified model for α decay and α capture (UMADAC). Compared theoretical half-lives extracted from empirical parametrization with experimental values. NUCLEAR REACTIONS 40,44Ca, 59Co, 208Pb, 209Bi(α, X); analyzed α-capture cross sections in the framework of unified model for α decay and α capture (UMADAC).
doi: 10.1103/PhysRevC.92.014602
2011AL03 Phys.Rev. C 83, 024913 (2011) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, A.A.Bickley, R.Bindel, A.Budzanowski, W.Busza, A.Carroll, Z.Chai, V.Chetluru, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, S.Gushue, C.Halliwell, J.Hamblen, G.A.Heintzelman, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, J.Katzy, N.Khan, J.Kotula, W.Kucewicz, P.Kulinich, C.M.Kuo, W.Li, W.T.Lin, C.Loizides, S.Manly, D.McLeod, J.Michalowski, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, I.C.Park, H.Pernegger, C.Reed, L.P.Remsberg, M.Reuter, C.Roland, G.Roland, L.Rosenberg, J.Sagerer, P.Sarin, P.Sawicki, I.Sedykh, W.Skulski, C.E.Smith, S.G.Steadman, P.Steinberg, G.S.F.Stephans, M.Stodulski, A.Sukhanov, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, B.Wadsworth, P.Walters, E.Wenger, F.L.H.Wolfs, B.Wosiek, K.Wozniak, A.H.Wuosmaa, B.Wyslouch Charged-particle multiplicity and pseudorapidity distributions measured with the PHOBOS detector in Au + Au, Cu + Cu, d + Au, and p + p collisions at ultrarelativistic energies
doi: 10.1103/PhysRevC.83.024913
2010AL01 Phys.Rev.Lett. 104, 062301 (2010) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, A.A.Bickley, R.Bindel, W.Busza, A.Carroll, Z.Chai, V.Chetluru, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, C.Halliwell, J.Hamblen, M.Hauer, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, N.Khan, P.Kulinich, C.M.Kuo, W.Li, W.T.Lin, C.Loizides, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, C.Roland, G.Roland, J.Sagerer, H.Seals, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, P.Walters, E.Wenger, F.L.H.Wolfs, B.Wosiek, K.Wozniak, B.Wyslouch High Transverse Momentum Triggered Correlations over a Large Pseudorapidity Acceptance in Au + Au Collisions at √ sNN = 200 GeV
doi: 10.1103/PhysRevLett.104.062301
2010AL04 Phys.Rev. C 81, 024904 (2010) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, R.Bindel, W.Busza, Z.Chai, V.Chetluru, E.Garcia, T.Gburek, K.Gulbrandsen, J.Hamblen, I.Harnarine, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, J.L.Kane, P.Kulinich, C.M.Kuo, W.Li, W.T.Lin, C.Loizides, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, E.Richardson, C.Roland, G.Roland, J.Sagerer, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, A.Szostak, M.B.Tonjes, A.Trzupek, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, P.Walters, E.Wenger, D.Willhelm, F.L.H.Wolfs, B.Wosiek, K.Wozniak, S.Wyngaardt, B.Wyslouch System size dependence of cluster properties from two-particle angular correlations in Cu+Cu and Au+Au collisions at √ sNN = 200 GeV
doi: 10.1103/PhysRevC.81.024904
2010AL08 Phys.Rev.Lett. 104, 142301 (2010) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, A.A.Bickley, R.Bindel, W.Busza, A.Carroll, Z.Chai, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, C.Halliwell, J.Hamblen, M.Hauer, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, N.Khan, P.Kulinich, C.M.Kuo, W.Li, W.T.Lin, C.Loizides, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, C.Roland, G.Roland, J.Sagerer, H.Seals, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, P.Walters, E.Wenger, F.L.H.Wolfs, B.Wosiek, K.Wozniak, B.Wyslouch Event-by-Event Fluctuations of Azimuthal Particle Anisotropy in Au+Au Collisions at √ sNN = 200 GeV
doi: 10.1103/PhysRevLett.104.142301
2008AL15 Phys.Rev. C 77, 061901 (2008) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, R.Bindel, W.Busza, Z.Chai, V.Chetluru, E.Garcia, T.Gburek, K.Gulbrandsen, J.Hamblen, I.Harnarine, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, J.L.Kane, P.Kulinich, C.M.Kuo, W.Li, W.T.Lin, C.Loizides, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, E.Richardson, C.Roland, G.Roland, J.Sagerer, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, A.Szostak, M.B.Tonjes, A.Trzupek, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, P.Walters, E.Wenger, D.Willhelm, F.L.H.Wolfs, B.Wosiek, K.Wozniak, S.Wyngaardt, B.Wyslouch Identified charged antiparticle to particle ratios near midrapidity in Cu+Cu collisions at √ sNN = 62.4 and 200 GeV
doi: 10.1103/PhysRevC.77.061901
2007AL31 Phys.Rev. C 75, 054913 (2007) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, R.Bindel, W.Busza, Z.Chai, V.Chetluru, E.Garcia, T.Gburek, K.Gulbrandsen, J.Hamblen, I.Harnarine, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, J.L.Kane, P.Kulinich, C.M.Kuo, W.Li, W.T.LIn, C.Lozides, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, E.Richardson, C.Roland, G.Roland, J.Sagerer, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephens, A.Sukhanov, A.Szopstak, M.B.Tonjes, A.Trzupek, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verier, G.I.Veres, P.Walters, E.Wenger, D.Willhelm, F.L.H.Wolfs, B.Wosiek, K.Wozniak, S.Wyngaardt, B.Wyslouch Cluster properties from two-particle angular correlations in p+p collisions at √ s = 200 and 410 GeV NUCLEAR REACTIONS 1H(p, X), E(cm)=200, 410 GeV; measured two particle angular correlations. Compared results to model calculations.
doi: 10.1103/PhysRevC.75.054913
2006AL11 Phys.Rev.Lett. 96, 212301 (2006) B.Alver, B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, R.Bindel, W.Busza, Z.Chai, V.Chetluru, E.Garcia, T.Gburek, K.Gulbrandsen, J.Hamblen, I.Harnarine, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, J.L.Kane, P.Kulinich, C.M.Kuo, W.Li, W.T.Lin, C.Loizides, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, E.Richardson, C.Roland, G.Roland, J.Sagerer, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, A.Szostak, M.B.Tonjes, A.Trzupek, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, P.Walters, E.Wenger, D.Willhelm, F.L.H.Wolfs, B.Wosiek, K.Wozniak, S.Wyngaardt, B.Wyslouch System Size and Centrality Dependence of Charged Hadron Transverse Momentum Spectra in Au + Au and Cu + Cu Collisions at √ sNN = 62.4 and 200 GeV NUCLEAR REACTIONS Cu(Cu, X), Au(Au, X), E(cm)=62.4, 200 GeV/nucleon; measured charged hadrons transverse momentum spectra; deduced system size and centrality dependence, nuclear modification factors.
doi: 10.1103/PhysRevLett.96.212301
2005BA17 Phys.Rev.Lett. 94, 082304 (2005) B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, A.A.Bickley, R.Bindel, W.Busza, A.Carroll, Z.Chai, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, C.Halliwell, J.Hamblen, M.Hauer, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, N.Khan, P.Kulinich, C.M.Kuo, W.T.Lin, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, C.Reed, C.Roland, G.Roland, J.Sagerer, H.Seals, I.Sedykh, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, E.Wenger, F.L.H.Wolfs, B.Wosiek, K.Wozniak, B.Wyslouch Centrality Dependence of Charged Hadron Transverse Momentum Spectra in Au + Au Collisions from √ sNN = 62.4 to 200 GeV NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=62.4 GeV/nucleon; measured charged hadrons transverse momentum spectra, centrality dependence; deduced medium modification factor. Comparison with data at higher energies.
doi: 10.1103/PhysRevLett.94.082304
2005BA32 Phys.Rev.Lett. 94, 122303 (2005) B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, R.R.Betts, A.A.Bickley, R.Bindel, A.Budzanowski, W.Busza, A.Carroll, Z.Chai, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, S.Gushue, C.Halliwell, J.Hamblen, M.Hauer, G.A.Heintzelman, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, J.Katzy, N.Khan, W.Kucewicz, P.Kulinich, C.M.Kuo, W.T.Lin, S.Manly, D.McLeod, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, I.C.Park, H.Pernegger, C.Reed, L.P.Remsberg, M.Reuter, C.Roland, G.Roland, L.Rosenberg, J.Sagerer, P.Sarin, P.Sawicki, H.Seals, I.Sedykh, W.Skulski, C.E.Smith, M.A.Stankiewicz, P.Steinberg, G.S.F.Stephans, A.Sukhanov, J.-L.Tang, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, S.S.Vaurynovich, R.Verdier, G.I.Veres, E.Wenger, F.L.H.Wolfs, B.Wosiek, K.Wozniak, A.H.Wuosmaa, B.Wyslouch Energy Dependence of Elliptic Flow over a Large Pseudorapidity Range in Au+Au Collisions at the BNL Relativistic Heavy Ion Collider NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=19.6, 62.4, 130, 200 GeV/nucleon; measured elliptic flow; deduced energy and pseudorapidity dependence.
doi: 10.1103/PhysRevLett.94.122303
2005BA83 Phys.Rev. C 72, 031901 (2005) B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, B.Becker, R.R.Betts, A.A.Bickley, R.Bindel, W.Busza, A.Carroll, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, S.Gushue, C.Halliwell, J.Hamblen, A.S.Harrington, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, N.Khan, P.Kulinich, C.M.Kuo, J.W.Lee, W.T.Lin, S.Manly, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, I.C.Park, H.Pernegger, C.Reed, C.Roland, G.Roland, J.Sagerer, P.Sarin, I.Sedykh, W.Skulski, C.E.Smith, P.Steinberg, G.S.F.Stephans, A.Sukhanov, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, R.Verdier, G.I.Veres, F.L.H.Wolfs, B.Wosiek, K.Wozniak, B.Wyslouch, J.Zhang Scaling of charged particle production in d+Au collisions at √ sNN = 200 GeV NUCLEAR REACTIONS 197Au(d, X), E(cm)=200 GeV/nucleon; analyzed charged particle pseudorapidity distribution, integrated multiplicities vs centrality.
doi: 10.1103/PhysRevC.72.031901
2004BA20 Braz.J.Phys. 34, 829 (2004) B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, B.Becker, R.R.Betts, A.A.Bickley, R.Bindel, A.Budzanowski, W.Busza, A.Carroll, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, S.Gushue, C.Halliwell, J.Hamblen, A.S.Harrington, G.A.Heintzelman, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, J.Katzy, N.Khan, W.Kucewicz, P.Kulinich, C.M.Kuo, J.W.Lee, W.T.Lin, S.Manly, D.McLeod, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, I.C.Park, H.Pernegger, C.Reed, L.P.Remsberg, M.Reuter, C.Roland, G.Roland, L.Rosenberg, J.Sagerer, P.Sarin, P.Sawicki, I.Sedykh, W.Skulski, C.E.Smith, P.Steinberg, G.S.F.Stephans, A.Sukhanov, J.-L.Tang, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, R.Verdier, G.I.Veres, F.L.H.Wolfs, B.Wosiek, K.Wozniak, A.H.Wuosmaa, B.Wyslouch, J.Zhang Recent Results from PHOBOS at RHIC NUCLEAR REACTIONS 197Au(d, X), (197Au, X), E(cm)=19.6, 130, 200 GeV/nucleon; measured charged particles pseudorapidity distributions, transverse momentum, yields; deduced nuclear modification factors.
doi: 10.1590/s0103-97332004000500032
2004BB20 Braz.J.Phys. 34, 829 (2004) B.B.Back, M.D.Baker, M.Ballintijn, D.S.Barton, B.Becker, R.R.Betts, A.A.Bickley, R.Bindel, A.Budzanowski, W.Busza, A.Carroll, M.P.Decowski, E.Garcia, T.Gburek, N.George, K.Gulbrandsen, S.Gushue, C.Halliwell, J.Hamblen, A.S.Harrington, G.A.Heintzelman, C.Henderson, D.J.Hofman, R.S.Hollis, R.Holynski, B.Holzman, A.Iordanova, E.Johnson, J.L.Kane, J.Katzy, N.Khan, W.Kucewicz, P.Kulinich, C.M.Kuo, J.W.Lee, W.T.Lin, S.Manly, D.McLeod, A.C.Mignerey, R.Nouicer, A.Olszewski, R.Pak, I.C.Park, H.Pernegger, C.Reed, L.P.Remsberg, M.Reuter, C.Roland, G.Roland, L.Rosenberg, J.Sagerer, P.Sarin, P.Sawicki, I.Sedykh, W.Skulski, C.E.Smith, P.Steinberg, G.S.F.Stephans, A.Sukhanov, J.-L.Tang, M.B.Tonjes, A.Trzupek, C.Vale, G.J.van Nieuwenhuizen, R.Verdier, G.I.Veres, F.L.H.Wolfs, B.Wosiek, K.Wozniak, A.H.Wuosmaa, B.Wyslouch, J.Zhang Recent Results from PHOBOS at RHIC NUCLEAR REACTIONS 197Au(d, X), (197Au, X), E(cm)=19.6, 130, 200 GeV/nucleon; measured charged particles pseudorapidity distributions, transverse momentum, yields; deduced nuclear modification factors.
doi: 10.1590/S0103-97332004000500032
1995LA20 Phys.Rev.Lett. 75, 1903 (1995) Yu.A.Lazarev, Yu.V.Lobanov, Yu.Ts.Oganessian, Yu.S.Tsyganov, V.K.Utyonkov, F.Sh.Abdullin, S.Iliev, A.N.Polyakov, J.Rigol, I.V.Shirokovsky, V.G.Subbotin, A.M.Sukhov, G.V.Buklanov, B.N.Gikal, V.B.Kutner, A.N.Mezentsev, I.M.Sedykh, D.V.Vakatov, R.W.Lougheed, J.F.Wild, K.J.Moody, E.K.Hulet New Nuclide 267108 Produced by the 238U + 34S Reaction NUCLEAR REACTIONS, ICPND 238U(34S, X)267Hs, E=186 MeV; measured Eα, Iα; deduced residual production σ. RADIOACTIVITY 267Hs(α) [from 238U(34S, X), E=186 MeV]; measured Eα, Iα, T1/2.
doi: 10.1103/PhysRevLett.75.1903
1994LA22 Phys.Rev.Lett. 73, 624 (1994) Yu.A.Lazarev, Yu.V.Lobanov, Yu.Ts.Oganessian, V.K.Utyonkov, F.Sh.Abdullin, G.V.Buklanov, B.N.Gikal, S.Iliev, A.N.Mezentsev, A.N.Polyakov, I.M.Sedykh, I.V.Shirokovsky, V.G.Subbotin, A.M.Sukhov, Yu.S.Tsyganov, V.E.Zhuchko, R.W.Lougheed, K.J.Moody, J.F.Wild, E.K.Hulet, J.H.McQuaid Discovery of Enhanced Nuclear Stability Near the Deformed Shells N = 162 and Z = 108 NUCLEAR REACTIONS 248Cm(22Ne, X), E=116, 121 MeV; measured Eα, Iα; deduced evidence for 265Sg, 266Sg. RADIOACTIVITY 265Sg, 266Sg(α); measured Eα, Iα; deduced T1/2, SF-decay upper limits. 262Rf [from 266Sg(α-decay)]; measured T1/2.
doi: 10.1103/PhysRevLett.73.624
1994LO27 J.Alloys and Compounds 213/214, 61 (1994) R.W.Lougheed, K.J.Moody, J.FD.Wild, E.K.Hulet, J.H.McQuaid, Yu.A.Lazarev, Yu.V.Lobanov, Yu.Ts.Oganessian, V.K.Utyonkov, F.Sh.Abdullin, G.V.Buklanov, B.N.Gikal, S.Iliev, A.N.Mezentsev, A.N.Polyakov, I.M.Sedykh, I.V.Shirokovsky, V.G.Subbotin, A.M.Sukhov, Yu.S.Tsyganov, V.E.Zhuchko Observation of enhanced nuclear stability near the 162 neutron shell RADIOACTIVITY 265,266Sg(α) [from 248Cm(22Ne, xn)]; measured Eα, T1/2. 262Rf(SF) [from 266Sg decay]; measured T1/2. Comparison with model predictions.
doi: 10.1016/0925-8388(94)90881-8
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