IREF= 1 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 93-93 A-Range= 237-237 E-Range= 0- 30 MeV Author(s)= P.G.Young and E.D.Arthur Reference= Proc.Int.Conf.Nucl.Data Sci.and Tech.,Julich (1992) p894 Summary= modification of potential by Haouat,Lachkar,Lagrange et al, NSE 81, (1982), especially for higher energy ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2 Neutron incident, CC vibrational model Potential is non-relativistic and non-dispersive Z-Range= 82-82 A-Range= 208-208 E-Range= 0-200 MeV Author(s)= H.Vonach,A.Pavlik,M.B.Chadwick,R.C.Haight,R.O.Nelson,S.A.Wender,P.G. Young Reference= Phys. Rev. C 50, 1952 (1994) Summary= Based on detailed fits to neutron data 8.5-10 MeV,simply extrapolated to lower energies and extended to higher energies. Reaction cross section deficient above 100 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 3 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 92-92 A-Range= 235-235 E-Range= 0- 30 MeV Author(s)= P.G.Young and E.D.Arthur Reference= Proc.Int.Conf.Nucl.Data Sci.and Tech.,Julich (1992) p894 Summary= modification of potential by Haouat,Lachkar,Lagrange et al, NSE 81, (1982), especially for higher energy ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 92-92 A-Range= 237-237 E-Range= 0- 30 MeV Author(s)= P.G.Young and E.D.Arthur Reference= LANL Report LA-UR-91-1424,894(1992) Summary= potential was inferred from the u-238 potential that covers the same energy range ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 92-92 A-Range= 238-238 E-Range= 0- 30 MeV Author(s)= P.G.Young and E.D.Arthur Reference= LANL Report LA-UR-91-1424,894(1992) Summary= modification of potential , NSE 81,49 (1982) , especially at higher energies ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 94-94 A-Range= 242-242 E-Range= 0- 20 MeV Author(s)= D.G.Madland and P.G.Young Reference= Report LA-7533-MS (1978) Summary= parameters were developed to provide Pu-242 total,elastic and inelastic neutron data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 7 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 94-94 A-Range= 239-239 E-Range= 0- 30 MeV Author(s)= P.G.Young and E.D.Arthur Reference= LANL Report LA-UR-91-1424,894(1992) Summary= Modification of potential by Haouat, Lachkar, Lagrange, et al., NSE 81 (1982) 49, especially above 20 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 8 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 95-95 A-Range= 241-243 E-Range= 0- 30 MeV Author(s)= P.G.Young and E.D.Arthur Reference= LANL Report LA-UR-95-3654, paper at RIPL CRP Mtg., Vienna, Oct.30-N ov.3,1995. Summary= based on pu-239 potential used for endf/b-vi with isospin corrections and some adjustments to better match tot-xs ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 90-95 A-Range= 230-250 E-Range= 0- 10 MeV Author(s)= D.G.Madland and P.G.Young Reference= Int.Conf.,Harwell UK,Sept. 25-29,1978 Summary= derived by fitting inelastic, elastic and total cross sections of several nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 10 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 54- 56 E-Range= 0- 52 MeV Author(s)= E.D.Arthur and P.G.Young Reference= LA-UR-95-3654 (1995),BNL-NCS-51245 (1980) p.731, LA-8626-MS (1980) Summary= Potential for neutron reactions on Fe-54 and Fe-56 nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 11 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 27-27 A-Range= 59- 59 E-Range= 0- 27 MeV Author(s)= E.D.Arthur, P.G.Young, and W.Matthes Reference= BNL-51245,p.751 (1980); Nucl.Sci.Eng.124,271(1996) Summary= potential developed for co-59 nuclide to analyze neutron reaction data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 12 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 30-30 A-Range= 57- 81 E-Range= 0- 20 MeV Author(s)= P.G.Young and D.Rutherford Reference= Report IAEA-TECDOC-483,167 (1988) Summary= potential developed for neutron interaction with zinc isotopes ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 13 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 39-39 A-Range= 89- 89 E-Range= 0- 21 MeV Author(s)= E.D.Arthur Reference= Nucl.Sci.Eng. 76,137 1980) Summary= potential developed for neutron interaction with y-89 nuclide ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 14 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 90- 90 E-Range= 0- 20 MeV Author(s)= E.D.Arthur Reference= Nucl.Sci.Eng. 76,137 (1980); LA-UR-94-3104 (1994) Summary= potential developed for neutron interaction with zr-90 nuclide ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 15 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6- 6 A-Range= 12- 12 E-Range= 0- 65 MeV Author(s)= M.B.Chadwick and P.G.Young Reference= Nucl.Sci.Eng. 123, 17 (1996) Summary= Calculation and evaluation of cross sections and kerma factors for neutrons up to 100 MeV on carbon. Potential based on experimental data and previous optical model analyses, especially Arthur and Dimbylow. See LA-UR-95-3654. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 16 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 7- 7 A-Range= 14- 14 E-Range= 0- 60 MeV Author(s)= M.B.Chadwick and P.G.Young Reference= Nucl.Sci.Eng. 123, 17 (1996) Summary= Calculation and evaluation of cross sections and kerma factors for neutrons up to 100 MeV on carbon. Potential based on experimental data and previous optical model analyses, especially Arthur and Islam. See LA-UR-95-3654. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 17 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 8- 8 A-Range= 16- 16 E-Range= 0- 50 MeV Author(s)= M.B.Chadwick and P.G.Young Reference= Nucl.Sci.Eng. 123, 17 (1996) Summary= Calculation and evaluation of cross sections and kerma factors for neutrons up to 100 MeV on carbon. Potential based on experimental data and previous optical model analyses, especially Arthur and Islam. See LA-UR-95-3654. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 18 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 19 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 20 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 21 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 79-79 A-Range= 197-197 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 100 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-92 A-Range= 40-238 E-Range= 10- 50 MeV Author(s)= F.D.Becchetti, Jr. and G.W.Greenlees Reference= Phys. Rev. 182,1190 (1969) Summary= derived by fitting total and diff. elastic cross sections of several nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 101 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 12-83 A-Range= 24-209 E-Range= 11- 11 MeV Author(s)= J.C.Ferrer,J.D.Carlson and J.Rapaport Reference= Nucl.Phys.A275,325(1977) Summary= Derived by fitting pure diff. elastic cross sections of several nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 102 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 82-82 A-Range= 206-208 E-Range= 5- 50 MeV Author(s)= R.W.Finlay et al. Reference= Phys. Rev. C 30, 796 (1984) Summary= derived by fitting elastic cross sections of lead ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 103 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 56- 56 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 104 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 54- 54 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 105 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 57- 57 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 106 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 58- 58 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 107 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 108 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 60- 60 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 109 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 61- 61 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 110 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 62- 62 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 111 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 64- 64 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 112 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 24-24 A-Range= 50- 50 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 113 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 24-24 A-Range= 53- 53 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 114 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 24-24 A-Range= 52- 52 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 115 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 24-24 A-Range= 54- 54 E-Range= 0-100 MeV Author(s)= A.Prince Reference= Int. Conf. on Nucl. Data, Antwerp ,1982 Summary= derived by applying sprt method and elastic and differential elastic cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 116 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-83 A-Range= 40-209 E-Range= 0- 5 MeV Author(s)= P.A.Moldauer Reference= Nucl. Phys. 47,65(1963) Summary= Based on analysis of low-energy neutron data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 117 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 60 MeV Author(s)= J.Petler,M.S.Islam, and R.W.Finlay Reference= Phys. Rev. C 32 ,673 (1985) Summary= potential specifically developed for neutron interaction with al-27 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 118 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 39-51 A-Range= 85-125 E-Range= 0- 5 MeV Author(s)= A.B.Smith,P.T.Guenther,J.F.Whalen Reference= Nucl. Phys. A415,1 (1984) Summary= Based on fits to measurements of total and differential elastic scattering cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 119 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 67-67 A-Range= 165-165 E-Range= 0- 30 MeV Author(s)= A.B.Smith Reference= Report ANL/NDM-151 (December, 2000) Summary= "Fast-Neutron Incident on Holmium". Based on analysis of differential elastic scattering cross section data at incident neutrons between 4.5-10.0 MeV measured at 40 angles or more. Pure coupled-channel analysis incorporating 7/2- ground-state rotational band. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 120 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and dispersive (Anal.Integr.) Z-Range= 67-67 A-Range= 165-165 E-Range= 0- 30 MeV Author(s)= A.B.Smith Reference= Report ANL/NDM-151 (December, 2000) Summary= "Fast-Neutron Incident on Holmium". Results from analyzing the same differential elastic scattering cross section data between 4.5-10.0 MeV as RIPL ref.#119 but using a dispersive coupled-channel potential incorporating 7/2- ground-state rotational band. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 121 Neutron incident, spherical nucleus model Potential is relativistic and dispersive (Anal.Integr.) Z-Range= 82-82 A-Range= 208-208 E-Range= 0- 80 MeV Author(s)= G.J.Weisel, W.Tornow et al Reference= Phys. Rev. C 54,2410-2428 (1996) Summary= A relativistic dispersive OMP for Pb-208. Fully constrained set w/Wso from 4th column, Table II(p.2420) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 122 Neutron incident, spherical nucleus model Potential is relativistic and dispersive (Anal.Integr.) Z-Range= 83-83 A-Range= 209-209 E-Range= 0- 80 MeV Author(s)= G.J.Weisel, W.Tornow et al Reference= Phys. Rev. C 54,2410-2428 (1996) Summary= A relativistic dispersive OMP for Bi-209. Fully constrained set w/Wso from 4th column, Table II(p.2420) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 123 Neutron incident, CC vibrational model Potential is non-relativistic and non-dispersive Z-Range= 62-62 A-Range= 148-150 E-Range= 0- 15 MeV Author(s)= M.T.McEllistrem,R.E.Shamu,J.Lachkar,G.Haouat,Ch.Lagrange,Y.Patin et al. Reference= Phys.Rev.C 15,927(1977). Summary= Deformation Effects in Neutron Scattering from the Sm Isotopes. Vibrational model used for 148,150Sm [RIPL#123]. Rotational model used for 150,152,154Sm [RIPL#124]. Saturation of Wd assumed at 10 MeV, as in earlier publication, Lagrange et al., Phys.Lett.58B,293(1975). ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 124 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 62-62 A-Range= 150-152 E-Range= 0- 15 MeV Author(s)= M.T.McEllistrem,R.E.Shamu,J.Lachkar,G.Haouat,Ch.Lagrange,Y.Patin et al. Reference= Phys.Rev.C 15,927(1977). Summary= Deformation Effects in Neutron Scattering from the Sm Isotopes. Vibrational model used for 148,150Sm [RIPL#123]. Rotational model used for 150,152,154Sm [RIPL#124]. Saturation of Wd assumed at 10 MeV, as in earlier publication, Lagrange et al., Phys.Lett.58B,293(1975). ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 125 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 54- 54 E-Range= 8- 14 MeV Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W .Seagondolla Reference= Nucl.Phys. A390,509(1982). Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. Spherical optical model potential from 54Fe experimental data [Table 4]. See RIPL#129 and 130 for global spherical potentials [Table 5]. Also, see RIPL#424-427 for vibrational model potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 126 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-26 A-Range= 56- 56 E-Range= 8- 14 MeV Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W .Seagondolla Reference= Nucl.Phys. A390,509(1982). Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. Spherical optical model potential from 56Fe experimental data [Table 4]. See RIPL#129 and 130 for global spherical potentials [Table 5]. Also, see RIPL#424-427 for vibrational model potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 127 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 29-29 A-Range= 63- 63 E-Range= 8- 14 MeV Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W .Seagondolla Reference= Nucl.Phys. A390,509(1982). Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. Spherical optical model potential from 63Cu experimental data [Table 4]. See RIPL#129 and 130 for global spherical potentials [Table 5]. Also, see RIPL#424-427 for vibrational model potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 128 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 29-29 A-Range= 65- 65 E-Range= 8- 14 MeV Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W .Seagondolla Reference= Nucl.Phys. A390,509(1982). Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. Spherical optical model potential from 65Cu experimental data [Table 4]. See RIPL#129 and 130 for global spherical potentials [Table 5]. Also, see RIPL#424-427 for vibrational model potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 129 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-29 A-Range= 54- 65 E-Range= 8- 30 MeV Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W .Seagondolla Reference= Nucl.Phys. A390,509(1982). Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. Global spherical potential [global set A in Table 5] See RIPL#125-128 for spherical potentials directly from data. Also, see RIPL#424-427 for vibrational model potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 130 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-29 A-Range= 54- 65 E-Range= 8- 30 MeV Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W .Seagondolla Reference= Nucl.Phys. A390,509(1982). Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. Global spherical potential [global set B in Table 5] See RIPL#125-128 for spherical potentials directly from data. Also, see RIPL#424-427 for vibrational model potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 131 Neutron incident, CC vibrational model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 60 E-Range= 0- 80 MeV Author(s)= P.P.Guss,R.C.Byrd,C.E.Floyd,C.R.Howell,K.Murphy,G.Tungate...,J.P.Del aroche Reference= Nucl.Phys. A438,187(1985). Summary= Cross Sections and Analyzing Powers for Fast-Neutron Scattering to the Ground and First Excited States of 58Ni and 60Ni. Vibrational model analysis with ECIS coupled-channels code [see discussion p.195 of Nucl.Phys. A438 on 2+ state reorientation matrix]. See RIPL#132 for spherical potential. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 132 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 60 E-Range= 0- 80 MeV Author(s)= P.P.Guss,R.C.Byrd,C.E.Floyd,C.R.Howell,K.Murphy,G.Tungate...,J.P.Del aroche Reference= Nucl.Phys. A438,187(1985). Summary= Cross Sections and Analyzing Powers for Fast-Neutron Scattering to the Ground and First Excited States of 58Ni and 60Ni. Spherical optical model analysis. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 133 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 22-22 A-Range= 44- 50 E-Range= 0- 20 MeV Author(s)= D.W.Muir and E.D.Arthur Reference= Journal of Nucl.Mat.122&123, 1058 (1984) Summary= Improved Activation Cross Sections for Vanadium and Titanium Spherical potentials used in calculations of fusion blankets. Titanium potential. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 134 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 23-23 A-Range= 50- 51 E-Range= 0- 20 MeV Author(s)= D.W.Muir and E.D.Arthur Reference= Journal of Nucl.Mat.122&123, 1058 (1984) Summary= Improved Activation Cross Sections for Vanadium and Titanium Spherical potentials used in calculations of fusion blankets. Vanadium potential. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 136 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 7- 7 A-Range= 14- 14 E-Range= 18- 60 MeV Author(s)= M.S.Islam,R.W.Finlay,J.S.Petler,J.Rapaport,R.Alarcon Reference= Phys.in Med.and Biol.33,315(1988). Summary= Neutron Scattering Cross Sections and Partial Kerma Values for Oxygen, Nitrogen and Calcium at 1853, 10 MeV < E < 80 MeV, based on fits to neutron and proton data. Note: Wd can be negative at energies near 80 MeV. To avoid negative Wd, run OMRETRIEVE with negative modtyp. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2300 Neutron incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV Author(s)= A.V.Ignatyuk,V.P.Lunev,Yu.N.Shubin,E.V.Gai,N.N.Titarenko,A.Ventura,W .Gudowski Reference= Nucl.Sci.Engr. 136, 340 (2000). Summary= Neutron Cross Section Evaluations for 238U Up to 150 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2301 Neutron incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-90 A-Range= 227-260 E-Range= 0-200 MeV Author(s)= A.V.Ignatyuk Reference= Priv.communication to NDS, BROND 2003 evaluations up to 150 MeV for 232 Th Summary= ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2302 Neutron incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-90 A-Range= 227-260 E-Range= 0-150 MeV Author(s)= A.V.Ignatyuk et al Reference= Nucl.Sc.&.Eng.142 (2002) 177-194 Summary= Requires an updated RIPL2 interfase code (R= r0 + r1*E + R2*E*E) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2303 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV Author(s)= A.V.Ignatyuk, E.V.Gai, V.P.Lunev, Yu.N.Shubin, N.N.Titarenko Reference= Progress Report IAEA RC 12571 (Sept. 2004) Summary= ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2404 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.J.van Wijk, J.P.Delaroche Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997) p.111. Summary= ECISVIEW: An interactive toolbox for optical model development. A preliminary nucleon potential from 0-200 MeV is described for 90Zr ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2405 Neutron incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003) [Global potential]. Summary= A new global neutron optical model potential for incident energies between 1 keV and 200 MeV and valid for Al through Bi. The potential is based on detailed fits of neutron total and elastic cross sections and elastic angular distributions with the ECISVIEW interactive code. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2406 Neutron incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 74-74 A-Range= 182-186 E-Range= 0- 16 MeV Author(s)= J.P.Delaroche,G.Haouat,J.Lachkar,Y.Patin,J.Sigaud,J.Chardine Reference= Phys. Rev. C 23, 136 (1981). Summary= Deformations, Moments, and Radii of 182,183,184,186W from Fast Neutron Scattering. Coupled-channels deformed - neutron and proton potentials via Lane model - valid to 16 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2407 Neutron incident, spherical nucleus model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 27-83 A-Range= 59-209 E-Range= 0-200 MeV Author(s)= B.Morillon and P.Romain Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006) Summary= The following modifications are required to the published OMP parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality gamma = 0.1165 - 1e-4*A A dispersive global spherical optical model potential for neutrons with incident energies between 1 keV and 200 MeV and valid for Co(A=59) up to Bi(A=209). ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2408 Neutron incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV Author(s)= R.Capote, E.Soukhovitski, S.Chiba, J.M.Quesada Reference= J. Nucl. Sc.&Tech. (Japan) 45 (2008) 333-340. Nice ND2007 proceeding s(pap#765). Summary= Dispersive coupled channel neutron OMP for incident energies between 1 keV and 200 MeV for actinides. Local Fermi energy used. Tested for 31 actinides. Th232; Pa231,232,233; U233,235,238; Pu239,240,242; Np237; Am241. Approximately Lane consistent (see PRC76 (2007) 057602). ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2409 Neutron incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba Reference= Unpublished. Summary= Lane consistent dispersive CC neutron OMP for incident energies between 1 keV and 200 MeV for actinides. Local Fermi energy used. Tested for 31 actinides. (See 5409 for the proton OMP) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2410 Neutron incident, spherical nucleus model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV Author(s)= B.Morillon and P.Romain Reference= Phys. Rev. C76, 044601 (2007) Summary= A dispersive global spherical optical model potential for neutrons (and protons) with incident energies between 1 keV and 200 MeV and valid for Al(A=27) up to Bi(A=209). Taken from the Table 1 for neutrons (M.R.07a) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2411 Neutron incident, spherical nucleus model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV Author(s)= B.Morillon and P.Romain Reference= Phys. Rev. C76, 044601 (2007) Summary= A dispersive global spherical optical model potential for neutrons (and protons) with incident energies between 1 keV and 200 MeV and valid for Al(A=27) up to Bi(A=209). Taken from the Table 2 for neutrons (M.R.07b) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2600 Neutron incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004). Summary= A new global coupled channel neutron OMP for incident energies between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 = -41.45 + 0.06667*232; Wd: 8.48744 = 17.38 - 0.03833*232; Updated parameters: VR1=0.024; VR2=1.7E-4; Smooth Fermi energy dependence. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2601 Neutron incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004). Summary= A new global coupled channel neutron OMP for incident energies between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 = -41.45 + 0.06667*232; Wd: 8.48744 = 17.38 - 0.03833*232; Updated parameters: VR1=0.024; VR2=1.7E-4; Local Fermi energy used. Recommended for Th230,232; U233,235,238; Pu239,240,242 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2602 Neutron incident, CC soft rotor model Potential is relativistic and non-dispersive Z-Range= 12-50 A-Range= 24-124 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, S. Chiba and J. Lee Reference= CP 769, Int.Conf.NDST, Santa Fe, USA, ed.by R.C.Haight et al, AIP 20 05, p. 1100. Summary= A global coupled channel soft rotor neutron OMP for incident energies between 1 keV and 200 MeV and valid for A=24-122 nuclei. Local Fermi energy used. Updated parameters: VR1=0.017; VR2=1.5E-4. Fitted to Mg24 26,Si28 30,S32,Ar40,Ca40,Ti48,Cr52,Fe54,56,Ni58 62,Zr90 92,Mo92-98 and Sn116 122 data. OPTMAN should be used. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 2700 Neutron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-83 A-Range= 40-210 E-Range= 0-155 MeV Author(s)= C.A.Engelbrecht and H.Fiedeldey Reference= Ann. Phys. 42,262-295 (1967) Summary= Derived from non-local formalism to fit total and nonelastic x-sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4000 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 25-26 A-Range= 54- 56 E-Range= 0- 28 MeV Author(s)= E.D.Arthur and P.G.Young Reference= LA-UR-95-3654 (1995),BNL-NCS-51245 (1980) p.731, LA-8626-MS (1980) Summary= Parameters developed for proton reactions with nuclides around Fe-54,Fe-56 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4001 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-27 A-Range= 59- 59 E-Range= 0- 23 MeV Author(s)= E.D.Arthur,P.G.Young,W.Matthes Reference= BNL-51245,p.751 (1980); Nucl.Sci.Eng.124,271(1996) Summary= Parameters to include proton emission competition in neutron induced cross-sections on Co-59 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4002 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 38-38 A-Range= 88- 89 E-Range= 0- 21 MeV Author(s)= E.D.Arthur Reference= Nucl.Sci.Eng. 76,137 (1980) Summary= Potential developed to analyze proton-induced reaction x-sections on Sr-88 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4003 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 39-39 A-Range= 89- 89 E-Range= 0- 21 MeV Author(s)= E.D.Arthur Reference= Nucl.Sci.Eng. 76,137 (1980) Summary= potential developed for proton reactions on Y-89 nuclide ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4004 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 79-79 A-Range= 197-197 E-Range= 0- 57 MeV Author(s)= P.G.Young and E.D.Arthur. Reference= LA-UR-84-2767(1984); LA-UR-94-3104(1994). Summary= Parameterization was developed for ENDF/B-VI to provide n,x gamma x-section data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4015 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6- 6 A-Range= 12- 12 E-Range= 0- 65 MeV Author(s)= M.B.Chadwick and P.G.Young Reference= Proc.Int. Particle Therapy Mtg. and PTCOG XXIV, 24-26 Apr. 1996,Detr oit,Mich. Summary= Proton Nuclear Interactions Up to 250 MeV for Radiation Transport Sumulations of Particle Therapy. Potential based on experimental data and previous optical model analyses, especially Arthur and Dimbylow. See LA-UR-95-3654. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4016 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 7- 7 A-Range= 14- 14 E-Range= 0- 70 MeV Author(s)= M.B.Chadwick and P.G.Young Reference= Proc.Int. Particle Therapy Mtg. and PTCOG XXIV, 24-26 Apr. 1996,Detr oit,Mich. Summary= Proton Nuclear Interactions Up to 250 MeV for Radiation Transport Sumulations of Particle Therapy. Potential based on experimental data and previous optical model analyses, especially Arthur and Islam. See LA-UR-95-3654. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4017 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 8- 8 A-Range= 16- 16 E-Range= 0- 50 MeV Author(s)= M.B.Chadwick and P.G.Young Reference= Proc.Int. Particle Therapy Mtg. and PTCOG XXIV, 24-26 Apr. 1996,Detr oit,Mich. Summary= Proton Nuclear Interactions Up to 250 MeV for Radiation Transport Sumulations of Particle Therapy. Potential based on experimental data and previous optical model analyses, especially Arthur and Islam. See LA-UR-95-3654. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4018 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4019 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4020 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4100 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 16-49 A-Range= 30-100 E-Range= 0- 22 MeV Author(s)= F.G.Perey Reference= Phys. Rev. 131,745 (1963) Summary= parameters developed to proton reaction data for medium mass nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4101 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-83 A-Range= 40-209 E-Range= 10- 50 MeV Author(s)= F.D.Becchetti Jr. and G.W.Greenlees Reference= Phys. Rev. 182,1190 (1969) Summary= diff. elastic and polarization data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4102 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6-82 A-Range= 12-208 E-Range= 30- 60 MeV Author(s)= J.J.H.Menet,E.E.Gross,J.J.Malanify, and A.Zucker Reference= Phys. Rev. C4,1114 (1971) Summary= parameters developed to provide total , elastic and inelastic data. Derived over 30-60 MeV energy range ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4108 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-82 A-Range= 48-208 E-Range= 25- 45 MeV Author(s)= D.M.Patterson et al Reference= Nucl. Phys. A263,261 (1976) Summary= global potential -energy and a dependent 25 to 45 MeV,A=48-208 (p,n)reactions (Following paper E = Ep - 0.84 Z/A**1/3 for the real potential !) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4109 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 39-39 A-Range= 89- 89 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4110 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 41-41 A-Range= 93- 93 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4111 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 45-45 A-Range= 103-103 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4112 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 46-46 A-Range= 105-105 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4113 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 47-47 A-Range= 107-107 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4114 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 47-47 A-Range= 109-109 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4115 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 48-48 A-Range= 110-110 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4116 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 48-48 A-Range= 111-111 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4117 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 48-48 A-Range= 113-113 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4118 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 48-48 A-Range= 114-114 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4119 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 49-49 A-Range= 115-115 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4120 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 50-50 A-Range= 116-116 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4121 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 50-50 A-Range= 122-122 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4122 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 50-50 A-Range= 124-124 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4123 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 52-52 A-Range= 128-128 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4124 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 52-52 A-Range= 130-130 E-Range= 1- 7 MeV Author(s)= C.H.Johnson et al Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979) Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4125 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 92- 92 E-Range= 2- 7 MeV Author(s)= D.S.Flynn et al Reference= Phys. Rev. C. 31, 87 (1985) Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n) excitation functions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4126 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 94- 94 E-Range= 2- 7 MeV Author(s)= D.S.Flynn et al Reference= Phys. Rev. C. 31, 87 (1985) Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n) excitation functions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4127 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 96- 96 E-Range= 2- 7 MeV Author(s)= D.S.Flynn et al Reference= Phys. Rev. C. 31, 87 (1985) Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n) excitation functions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4128 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 42-42 A-Range= 95- 95 E-Range= 2- 7 MeV Author(s)= D.S.Flynn et al Reference= Phys. Rev. C. 31, 87 (1985) Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n) excitation functions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4129 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 42-42 A-Range= 98- 98 E-Range= 2- 7 MeV Author(s)= D.S.Flynn et al Reference= Phys. Rev. C. 31, 87 (1985) Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n) excitation functions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4130 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 42-42 A-Range= 100-100 E-Range= 2- 7 MeV Author(s)= D.S.Flynn et al Reference= Phys. Rev. C. 31, 87 (1985) Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n) excitation functions ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4131 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 12-82 A-Range= 24-208 E-Range= 80-180 MeV Author(s)= P.Schwandt, H.O.Meyer, W.W.Jacobs, A.D.Bacher, S.E.Vigdor, M.D.Kaitc huck et al. Reference= Phys. Rev. C. 26, 55 (1982) Summary= Analyzing power of proton-nucleus elastic scattering between 80 and 180 MeV. Based on systematic analysis of elastic scattering of polarized protons between 80-180 MeV for a number of target nuclei. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4300 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV Author(s)= A.V.Ignatyuk,V.P.Lunev,Yu.N.Shubin,E.V.Gai,N.N.Titarenko,A.Ventura,W .Gudowski Reference= Nucl.Sci.Eng. 136, 340 (2000). Summary= Neutron Cross Section Evaluations for 238U Up to 150 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4301 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-90 A-Range= 227-260 E-Range= 0-200 MeV Author(s)= A.V.Ignatyuk Reference= Priv.communication to NDS, BROND 2003 evaluations up to 150 MeV for 232 Th Summary= ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4302 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-90 A-Range= 227-260 E-Range= 0-150 MeV Author(s)= A.V.Ignatyuk et al Reference= Nucl.Sc.&.Eng.142 (2002) 177-194 Summary= Requires an updated RIPL2 interfase code (R= r0 + r1*E + R2*E*E) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4303 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 90-92 A-Range= 228-234 E-Range= 0-200 MeV Author(s)= A.V.Ignatyuk, E.V.Gai, V.P.Lunev, Yu.N.Shubin, N.N.Titarenko Reference= Progress Report IAEA RC 12571 (Sept. 2004) Summary= ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4416 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4417 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 14-14 A-Range= 28- 28 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4418 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 20-20 A-Range= 40- 40 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4419 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 26-26 A-Range= 54- 54 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4420 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 26-26 A-Range= 56- 56 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4421 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4422 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 28-28 A-Range= 60- 60 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4423 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 28-28 A-Range= 62- 62 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4424 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 29-29 A-Range= 63- 63 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4425 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 28-28 A-Range= 64- 64 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4426 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4427 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 50-50 A-Range= 120-120 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4428 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 82-82 A-Range= 208-208 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4429 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 83-83 A-Range= 209-209 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003). Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV. Based on detailed fits of neutron total and nucleon elastic cross sections and angular distributions with the ECISVIEW interactive code. See ref # 5405 for a global potential with same methodology. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4430 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 45-45 A-Range= 100-104 E-Range= 0-200 MeV Author(s)= L.C.Mihailescu,I.Sirakov,R.Capote,E.Soukhovitski, et al. Reference= Proc.Int.Conf. on NDST, ND2007, Nice, France, #617, DOI: 10.1051/nda ta:07617 Summary= Geometry is different for Vhf and Wv. Dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV for Rh-103 (based on 1479). pot(1,1,9) = Ccoul/1.73*rc = 0.63208; rc=1.0935 Ccoul = 1.0 ac=0.36 Local Fermi energy used. Recommended for Rh-100 - 104 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4431 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 74-74 A-Range= 178-183 E-Range= 0-200 MeV Author(s)= R.Capote, E.Soukhovitski, J.M. Quesada, S. Chiba Reference= Unpublished. Summary= A dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV valid for W-182,183. (proton potential for 1480) pot(1,1,9) = Ccoul/1.73*rc = 1.22763; rc=1.0619 Ccoul = 2.0 ac=0.64 Local Fermi energy used. Recommended for W-178,W-183 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4432 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 73-73 A-Range= 178-186 E-Range= 0-200 MeV Author(s)= R.Capote, E.Soukhovitski, J.M. Quesada, S. Chiba Reference= Unpublished. Summary= A dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV valid for tantalum pot(1,1,9) = Ccoul/1.73*rc = 1.22763; rc=1.0619 Ccoul = 2.0 ac=0.64 Local Fermi energy used. Used in IAEA tungsten evaluation (proton emission). ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4433 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 79-79 A-Range= 195-200 E-Range= 0-200 MeV Author(s)= E.Soukhovitskii and R.Capote Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Lane-consistent dispersive CC proton OMP for incident energies between 1 keV and 200 MeV for gold. Local Fermi energy used. See 1483 for neutron OMP. Geometry is different for Vhf and Wv. Ep = Ep - 0.92999 Z/A**1/3 See RIPL paper, Table 6. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4434 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 25-25 A-Range= 50- 56 E-Range= 0-200 MeV Author(s)= E.Soukhovitskii and R.Capote Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Lane-consistent dispersive CC proton OMP for incident energies between 1 keV and 200 MeV for Mn-55. Local Fermi energy used. See 1484 for neutron OMP. Geometry is different for Vhf and Wv. Ep = Ep - 1.1 Z/A**1/3. See RIPL paper, Table 6. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4435 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 45-45 A-Range= 100-104 E-Range= 0-200 MeV Author(s)= E.Soukhovitskii and R.Capote Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Lane-consistent dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV. Recommended for Rh-100 - 104. Local Fermi energy used. See 1485 for neutron OMP. Ep = Ep - 1.10000 Z/A**1/3 See RIPL paper, Table 6. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4601 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV Author(s)= V.M.Maslov, Yu.V.Porodzinskij, N.A.Tetereva, M.Baba, A.Hasegawa Reference= Nucl. Phys. A736, 77-92 (2004) Summary= Rigid rotor OMP valid for incident energies from 1 kev to 200 MeV. Best description of the total cross section data for U238 Wd: 10.915 = 9.315 + 0.08*20 ; Wv50: 3.75 = 5 - 0.025*50; Wv80: 4.15 = 5.75 - 0.02*80; ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4602 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV Author(s)= V.M.Maslov, Yu.V.Porodzinskij, N.A.Tetereva, M.Baba, A.Hasegawa Reference= Nucl. Phys. A736, 77-92 (2004) Summary= Rigid rotor OMP valid for incident energies from 1 kev to 200 MeV. Best description of the fission cross section data for U238 Wd14: 10.123 = 8.443 + 0.12*14 ; Wd50: 12.443 = 8.443 + 0.08*50; Wv14: -1.12=-14*0.08; Wv50: -2.12=2.88 - 0.1*50; Wv80: 4.28=5.88 - 0.02*80; ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4603 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV Author(s)= V.M.Maslov Reference= Private communication to NDS (Updated on Dec.22,2004) Summary= Best description of the total cross section data for Th232 rc taken according to Koning recommendations ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4604 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV Author(s)= V.M.Maslov Reference= Private communication to NDS (Updated on Dec.22, 2004) Summary= Best description of the fission cross section data for Th232 rc taken according to Koning recommendations ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4605 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 90-92 A-Range= 228-234 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, R. Capote, J.M.Quesada, S.Chiba Reference= Unpublished. Summary= A dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV valid for Th. pot(1,1,9) = Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 ac=0.542 Local Fermi energy used. Recommended for Th232,U233 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4606 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 92-92 A-Range= 236-240 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba Reference= Unpublished. Summary= A dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV valid for U238. pot(1,1,9) = Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 acoul=0.542 Local Fermi energy used. Recommended for U238. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4607 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 92-92 A-Range= 232-234 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba Reference= Unpublished. Summary= A dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV valid for U-233. pot(1,1,9) = Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 acoul=0.542 Local Fermi energy used. Recommended for U233 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4608 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 90-91 A-Range= 228-234 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba Reference= Phys.Rev.C72 (2005) 024604 Summary= A dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV valid for Th, fitted to the new average cross section derived by Geel g roup from 1-150 keV. Local Fermi energy used. Recommended for Th232,Pa231,233. pot(1,1,9) = Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 acoul = 0.545 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4609 Proton incident, CC soft rotor model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 40-40 A-Range= 90- 92 E-Range= 0-200 MeV Author(s)= E.Soukhovitskii and R. Capote Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Lane-consistent dispersive CC proton OMP for incident energies between 1 keV and 200 MeV for Zr isotopes. Recommended for Zr-90,92,94,96. Local Fermi energy used. See 4609 for proton OMP. Soft rotor. See RIPL paper, Table 6. Following paper E = Ep - 1.1 * Z/A**1/3. See 609 for neutron potential. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4610 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 72-74 A-Range= 174-186 E-Range= 0-200 MeV Author(s)= E.Soukhovitskii and R. Capote Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Lane consistent dispersive CC proton OMP for incident energies between 1 keV and 200 MeV for Hf-W-Ta isotope. Recommended for Hf-178,180, Ta-181, all W. Local Fermi energy used. See 610 for neutron OMP. Soft rotor. OPTMAN should be used. Ep = Ep - 1.33 Z/A**1/3, rc=1.0626, ac=0.64. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4650 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 21-21 A-Range= 45- 45 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4651 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-20 A-Range= 48- 48 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4652 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 23-23 A-Range= 51- 51 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4653 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 24-24 A-Range= 54- 54 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4654 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 27-27 A-Range= 59- 59 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4655 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 61- 61 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4656 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 29-29 A-Range= 65- 65 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4657 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 31-31 A-Range= 71- 71 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4658 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 33-33 A-Range= 75- 75 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4659 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 34-34 A-Range= 80- 80 E-Range= 3- 5 MeV Author(s)= S.Kailas et al Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986) Summary= proton optical potential below 5 MeV for medium-weight nuclei A=45-80 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4660 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 19-19 A-Range= 41- 41 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4661 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 21-21 A-Range= 45- 45 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4662 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-20 A-Range= 48- 48 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4663 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 22-22 A-Range= 49- 49 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4664 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 23-23 A-Range= 51- 51 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4665 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 25-25 A-Range= 55- 55 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4666 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 27-27 A-Range= 59- 59 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4667 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 61- 61 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4668 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 29-29 A-Range= 65- 65 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4669 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 30-30 A-Range= 68- 68 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4670 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 31-31 A-Range= 71- 71 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4671 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 33-33 A-Range= 75- 75 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4672 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 34-34 A-Range= 80- 80 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4673 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 39-39 A-Range= 89- 89 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4674 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 41-41 A-Range= 93- 93 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4675 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 42-42 A-Range= 96- 96 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4676 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 42-42 A-Range= 98- 98 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4677 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 45-45 A-Range= 103-103 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4678 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 46-46 A-Range= 105-105 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4679 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 47-47 A-Range= 107-107 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4680 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 47-47 A-Range= 109-109 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4681 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 48-48 A-Range= 110-110 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4682 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 49-49 A-Range= 115-115 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4683 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 50-50 A-Range= 120-120 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4684 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 50-50 A-Range= 124-124 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4685 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 52-52 A-Range= 128-128 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 4686 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 52-52 A-Range= 130-130 E-Range= 1- 7 MeV Author(s)= Y.P.Viyogi Reference= Ph.D Thesis (Calcutta University 1983) Summary= proton optical potential below 7 MeV for nuclei A=40-130 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5001 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 6-82 A-Range= 12-208 E-Range= 50-400 MeV Author(s)= D.G.Madland Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997) p.129. Summary= Update of Semmering potential [NEANDC-245 U (1988)] to include generalized imag. diff. parameter. Global pot for incid. neuts and prots. Requires OM code with relativistic kine. & total pot must be multiplied by 1 + E/(E+2*mc**2) where E,m are for incident particle and E = total cm kinetic energy. Checked by author. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5002 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 74-74 A-Range= 182-186 E-Range= 0-100 MeV Author(s)= P.G.Young,E.D.Arthur,M.Bozian,T.R.England,G.M.Hale,R.J.LaBauve,R.C.L ittle,et al. Reference= LANL Report LA-11753-MS (1990); see also LA-8630-PR,p2 (1980) Summary= parameters are based on neutron elastic ,inelastic,total and differential data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5003 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 67-69 A-Range= 165-169 E-Range= 0-100 MeV Author(s)= E.D.Arthur and C.Philis Reference= Report LA-8630-PR,p2 (1980) Summary= Parameters are based on fits to 169Tm low-energy resonance data and total cross sections, plus fits to 11-MeV neutron scattering on 165Ho. Lane model used to relate n and p potentials. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5004 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 63-63 A-Range= 151-153 E-Range= 0- 20 MeV Author(s)= R.Macklin and P.G.Young Reference= Nucl.Sci.Eng. 95,189(1987) Summary= parameterization was developed to provide radiative capture x-sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5005 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 75-75 A-Range= 185-187 E-Range= 0- 20 MeV Author(s)= R.Macklin and P.G.Young Reference= Nucl.Sci.Eng. 97,239(1987) Summary= parameterization was developed to provide radiative capture cross sections ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5006 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV Author(s)= P.G.Young Reference= LANL Progress Report LA-11972-PR (1990) p.9 Summary= Modification of potential by Haouat, Lachkar, Lagrange, et al., NSE 81 (1982) 49. Extension above 20 MeV is based on total cross section data from WNR. Reaction cross section is too high by almost 20% at 200 MeV - modification needed above 20 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5100 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-83 A-Range= 40-209 E-Range= 16- 65 MeV Author(s)= R.L.Varner,W.J.Thompson,T.L.McAbee,E.J.Ludwig,T.B.Clegg Reference= Phys. Rep. 201,57 (1991) Summary= Total x-section and polarization data, together with (p,p) and (n,n) data, were fit ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5101 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 26-82 A-Range= 54-208 E-Range= 10- 80 MeV Author(s)= R.L.Walter and P.P.Guss Reference= Rad. Effects 95, 73 (1986) [1985 Santa Fe Conf. Proc.] Summary= A Global Optical Model for Neutron Scattering for A>53, 10 MeV < E < 80 MeV, based on fits to neutron and proton data. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5404 Proton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.J.van Wijk, J.P.Delaroche Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997) p.111. Summary= ECISVIEW: An interactive toolbox for optical model development. A preliminary nucleon potential from 0-200 MeV is described for 90Zr ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5405 Proton incident, spherical nucleus model Potential is relativistic and non-dispersive Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV Author(s)= A.J.Koning, J.P.Delaroche Reference= Nucl. Phys. A713, 231 (2003) [Global potential]. Summary= A new global proton optical model potential for incident energies between 1 keV and 200 MeV and valid for Al through Bi. The potential is based on detailed fits of proton elastic cross sections and elastic angular distributions with the ECISVIEW interactive code. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5406 Proton incident, CC rigid rotor deformed model Potential is non-relativistic and non-dispersive Z-Range= 74-74 A-Range= 182-186 E-Range= 0- 16 MeV Author(s)= J.P.Delaroche,G.Haouat,J.Lachkar,Y.Patin,J.Sigaud,J.Chardine Reference= Phys. Rev. C 23, 136 (1981). Summary= Deformations, Moments, and Radii of 182,183,184,186W from Fast Neutron Scattering. Coupled-channels deformed - neutron and proton potentials via Lane model - valid to 16 MeV. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5408 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV Author(s)= R.Capote, E.Soukhovitski, S. Chiba, J.M.Quesada Reference= J. Nucl. Sc.&Tech. (Japan) 45 (2008) 333-340. Nice ND2007 proceeding s(pap#765). Summary= Dispersive coupled channel proton OMP for incident energies between 1 keV and 200 MeV for actinides. Local Fermi energy used. Tested for 31 actinides. Th232; Pa231,232,233; U233,235,238; Pu239,240,242; Np237; Am241. pot(1,1,9) = Ccoul/1.73*rc = 1.13999; rc=1.2174 Ccoul = 1.62 acoul = 0.551 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5409 Proton incident, CC rigid rotor deformed model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba Reference= Unpublished. Summary= Lane consistent dispersive CC proton OMP for incident energies between 1 keV and 200 MeV for actinides. Local Fermi energy used. Tested for 31 actinides. Ccoul = 1.10, acoul = 0.40. Following paper E = Ep - Ccoul * Z/A**1/3. See 2409 for neutron potential. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5410 Proton incident, spherical nucleus model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV Author(s)= B.Morillon and P.Romain Reference= Phys. Rev. C76, 044601 (2007) Summary= A dispersive global spherical optical model potential for neutrons (and protons) with incident energies between 1 keV and 200 MeV and valid for Al(A=27) up to Bi(A=209). Taken from the Table 1 for protons (M.R.07a). Coulomb correction is constant and equal to 1.15Z/RC with RC=rc*A^(1/3). pot(1,1,9)=1.15/1.73=0.66474 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5411 Proton incident, spherical nucleus model Potential is relativistic and dispersive+SO(Anal.Integr.) Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV Author(s)= B.Morillon and P.Romain Reference= Phys. Rev. C76, 044601 (2007) Summary= A dispersive global spherical optical model potential for neutrons (and protons) with incident energies between 1 keV and 200 MeV and valid for Al(A=27) up to Bi(A=209). Taken from the Table 2 for protons (M.R.07b) + Table 1. Coulomb correction is constant and equal to 1.15Z/RC with RC=rc*A^(1/3). ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5501 Proton incident, spherical nucleus model Potential is non-relativistic and dispersive+SO(Anal.Integr.) Z-Range= 12-94 A-Range= 24-240 E-Range= 0-200 MeV Author(s)= Xiaohua Li, Chonghai Cai Reference= Nucl. Phys. A801, 43-67 (2008). Summary= A global dispersive spherical proton OMP for incident energies between 1 keV and 200 MeV. Local Fermi energy dependence. Non-relativistic OMP. Published potential reffited due to errata in OMP definition. Parameter set corresponding to the LAB energies (priv. comm. by authors) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5600 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004). Summary= A new global coupled channel proton OMP for incident energies between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 = -41.45 + 0.06667*232; Ccoul=1; pot(1,1,9)=Ccoul/1.73*rc=0.730809; Wd: 8.48744=17.38-0.03833*232; ac=0.343 Updated parameters: VR1=0.024; VR2=1.7E-4; Smooth Fermi energy dependence. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5601 Proton incident, CC rigid rotor deformed model Potential is relativistic and non-dispersive Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004). Summary= A new global coupled channel proton OMP for incident energies between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 = -41.45 + 0.06667*232; Ccoul=1; pot(1,1,9)=Ccoul/1.73*rc=0.730809; Wd: 8.48744=17.38-0.03833*232; ac=0.343 Updated parameters: VR1=0.024; VR2=1.7E-4; Local Fermi energy dependence. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 5602 Proton incident, CC soft rotor model Potential is relativistic and non-dispersive Z-Range= 12-50 A-Range= 24-124 E-Range= 0-200 MeV Author(s)= E.Soukhovitski, S. Chiba and J. Lee Reference= CP 769, Int.Conf.NDST, Santa Fe, USA, ed.by R.C.Haight et al, AIP 20 05, p. 1100. Summary= A global coupled channel soft rotor proton OMP for incident energies between 1 keV and 200 MeV and valid for A=24-122 nuclei. Local Ef used. Updated parameters: VR1=0.017; VR2=1.5E-4. Fitted to Mg24 26,Si28 30,S32,Ar40,Ca40,Ti48,Cr52,Fe54,56,Ni58 62,Zr90 92,Mo92-98 and Sn116 122 data.pot(1,1,9)=Ccoul*0.832*rc=0.944431 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6100 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-83 A-Range= 40-209 E-Range= 8- 13 MeV Author(s)= J.M.Lohr and W.Haeberli Reference= Nucl. Phys. A232,381(1974) Summary= Parameters developed to provide data for differential ela and inelastic data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6101 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-82 A-Range= 40-208 E-Range= 11- 27 MeV Author(s)= C.M.Perey and F.G.Perey Reference= Phys. Rev. 132,755 (1963) Summary= diff. elastic x-section data and other measured data analysis ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6112 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-20 A-Range= 40- 40 E-Range= 11- 90 MeV Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj. Reference= Phys.Rev.C21,2253(1980). Summary= Global optical model potential for elastic deuteron scattering from 12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv, Wd, and a imaginary terms in order to get into RIPL2 format. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6113 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 11- 90 MeV Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj. Reference= Phys.Rev.C21,2253(1980). Summary= Global optical model potential for elastic deuteron scattering from 12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv, Wd, and a imaginary terms in order to get into RIPL2 format. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6114 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 40-40 A-Range= 90- 90 E-Range= 11- 90 MeV Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj. Reference= Phys.Rev.C21,2253(1980). Summary= Global optical model potential for elastic deuteron scattering from 12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv, Wd, and a imaginary terms in order to get into RIPL2 format. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6115 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 50-50 A-Range= 120-120 E-Range= 11- 90 MeV Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj. Reference= Phys.Rev.C21,2253(1980). Summary= Global optical model potential for elastic deuteron scattering from 12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv, Wd, and a imaginary terms in order to get into RIPL2 format. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6116 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 82-82 A-Range= 208-208 E-Range= 11- 90 MeV Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj. Reference= Phys.Rev.C21,2253(1980). Summary= Global optical model potential for elastic deuteron scattering from 12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv, Wd, and a imaginary terms in order to get into RIPL2 format. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6200 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6-92 A-Range= 12-238 E-Range= 1-200 MeV Author(s)= Haixia An and Chonghai Cai. Reference= Phys. Rev. C73, 054605 (2006) Summary= Elastic deuteron scattering and deuteron reaction cross sections for energies up to 183 MeV. Vc=0.642/0.4=1.605 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6201 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6-83 A-Range= 12-209 E-Range= 1-200 MeV Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen. Reference= Phys.Rev.C74, 044615 (2006) Summary= Elastic deuteron scattering and deuteron reaction cross sections for energies up to 200 MeV. Vc=1.0584/0.4=2.646 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6202 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 3- 3 A-Range= 6- 7 E-Range= 1-200 MeV Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen. Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Elastic deuteron scattering and deuteron reaction cross sections for energies up to 200 MeV on Lithium. Local potential. Vc=0.7593/0.4=1.89825. See theory in Phys. Rev. C74 044615 (2006) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6203 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 4- 4 A-Range= 8- 10 E-Range= 1-200 MeV Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen. Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Elastic deuteron scattering and deuteron reaction cross sections for energies up to 200 MeV on Be-9. Local potential. Vc=1.7719/0.4=4.42975. See theory in Phys. Rev. C74 044615 (2006) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6204 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6- 6 A-Range= 11- 13 E-Range= 1-200 MeV Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen. Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper) Summary= Elastic deuteron scattering and deuteron reaction cross sections for energies up to 200 MeV on C-12. Local potential. Vc=1.4140/0.4=3.535. See theory in Phys. Rev. C74 044615 (2006) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 6400 Deuteron incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 6-82 A-Range= 12-208 E-Range= 20-100 MeV Author(s)= J.Bojowald et al Reference= Phys. Rev. C 38,1153(1988) Summary= Elastic deuteron scattering for energies up to 100 MeV ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 7100 Triton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-82 A-Range= 40-208 E-Range= 1- 40 MeV Author(s)= F.D.Becchetti Jr. and G.W.Greenlees Reference= Ann. Rept. J.H.Williams Lab., Univ. Minnesota (1969) Summary= Parameterization developed to analyze measured data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 7200 Triton incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 13-90 A-Range= 27-232 E-Range= 1- 40 MeV Author(s)= Xiaohua Li, Chuntian Liang, Chonghai Cai. Reference= Nucl.Phys.A789, 103-113(2007) Summary= Elastic triton scattering for Al-27, F-19 and Ca-Th nuclei up to 40 MeV. Vc=1.0474/0.4=2.6185 ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 8100 He-3 incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-82 A-Range= 40-208 E-Range= 1- 40 MeV Author(s)= F.D.Becchetti Jr. and G.W.Greenlees Reference= Ann. Rept. J.H.Williams Lab., Univ. Minnesota (1969) Summary= Parameters developed to analyze measured data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 8101 He-3 incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-20 A-Range= 40- 40 E-Range= 21- 84 MeV Author(s)= H.H.Chang et al Reference= Nucl. Phys. A297,105 (1978) Summary= Helium-3 on 40Ca and 58Ni energies 27.7,51.4,73.2,83.5 MeV ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 8102 He-3 incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 22- 84 MeV Author(s)= H.H.Chang et al Reference= Nucl. Phys. A297,105 (1978) Summary= Helium-3 on 40Ca and 58Ni energies 27.7,51.4,73.2,83.5 MeV ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9000 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 13-26 A-Range= 27- 56 E-Range= 1-100 MeV Author(s)= E.D.Arthur and P.G.Young Reference= Report LA-8636-MS(ENDF-304) (1980) Summary= potential developed to analyze alpha reaction data for medium nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9001 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 27-27 A-Range= 59- 59 E-Range= 1-100 MeV Author(s)= E.D.Arthur,P.G.Young,W.Matthes Reference= Report BNL-51245,751(1980) Summary= potential developed for alpha reaction data for co-59 and other nuclides in the vicinity ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9018 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9019 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 28-28 A-Range= 58- 58 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9020 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV Author(s)= R.C.Harper and W.L.Alford Reference= J.Phys.G:Nucl.Phys. 8, 153(1982) Summary= Experimental and theoretical neutron cross sections at 14 MeV. Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for incident neutrons, protons, and alphas. ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9100 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 8-82 A-Range= 16-208 E-Range= 1- 25 MeV Author(s)= L.McFadden and G.R.Satchler Reference= Nucl. Phys. 84, 177 (1966) Summary= parameters developed to analyze elastic scattering data for several nuclides ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9101 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 10-92 A-Range= 20-235 E-Range= 1- 46 MeV Author(s)= J.R.Huizenga and G.Igo Reference= Nucl. Phys. 29,462 (1962) Summary= total x-section and transmission coefficient calculations for several nuclides used to determine potential ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9400 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 20-45 A-Range= 40-100 E-Range= 1- 30 MeV Author(s)= B.Strohmaier et al Reference= IAEA Advisory Group Meeting, Rad.Damage 1981 Summary= For structural materials based on (n,nx),(n,px) and (n,alpha x) data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9401 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 22-30 A-Range= 37- 86 E-Range= 20- 30 MeV Author(s)= O.F.Lemos Reference= Orsay, Series A ,No.136 (1972) Summary= Diffusion Elastique de Particules Alpha de 21 a 29.6 MeV de la Region Ti-Zn, Orsay, France ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9600 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 8-96 A-Range= 16-250 E-Range= 1- 73 MeV Author(s)= V.Avrigeanu,P.E.Hodgson, and M.Avrigeanu Reference= Report OUNP-94-02 (1994) , Phys. Rev. C49,2136 (1994) Summary= global potential - extension of potential by Nolte et al ref. Phys. Rev. c36,1312 (1987) ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9601 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 39-50 A-Range= 89-124 E-Range= 1- 32 MeV Author(s)= M.Avrigeanu,W.von Oertzen,F.L.Roman, and V.Avrigeanu Reference= Progress Report IAEA RC 12422/R1 (2004), see also Nucl. Phys. A723,1 04(2003) Summary= Regional potential parameters based on alpha-particle elastic differential data ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ IREF= 9603 Alpha incident, spherical nucleus model Potential is non-relativistic and non-dispersive Z-Range= 21-21 A-Range= 44- 46 E-Range= 1- 50 MeV Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert zen Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris , Nov. 2009. Summary= Regional parameter set for alpha-particles, from analysis of elastic-scattering data for nuclei within 50