NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.C.Lagunas-Solar Found 21 matches. 1996LA36 Trans.Amer.Nucl.Soc. 74, 134 (1996) M.C.Lagunas-Solar, N.X.Zeng, I.Mirshad, C.M.Castaneda Cyclotron Production of Molybdenum-99 via Proton-Induced Uranium-238 Fission NUCLEAR REACTIONS 238U(p, F)99Mo, E=12.0-67.5 MeV; measured production σ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0961. 1995LA27 Appl.Radiat.Isot. 46, 833 (1995) M.C.Lagunas-Solar, O.F.Carvacho Cyclotron Production of PET Radionuclides: No-carrier-added fluorine-18 with high-energy protons on natural neon gas targets NUCLEAR REACTIONS, ICPND Ne(p, X)18F, E=22-68 MeV; measured residual production yields, thin targets; calculated thick target yields, total σ.
doi: 10.1016/0969-8043(95)00148-7
1993LA29 Radiochim.Acta 60, 57 (1993) Theoretical and Experimental Excitation Functions for Proton Induced Nuclear Reactions on Z = 10 to Z = 82 Target Nuclides NUCLEAR REACTIONS, ICPND Ne, 23Na, Mg(p, X)18F, 27Al, Mg(p, X)22Na, Mg, 27Al(p, X)24Na, E=20-70 MeV; Cl(p, X)34Cl, 56Fe(p, n), 59Co(p, X)56Co/57Co/54Mn/57Ni, 67Zn(p, n), (p, 2n), E=5-70 MeV; 66Zn(p, n), 68Zn(p, 2n), (p, 3n), Rb(p, X)83Rb/84Rb/86Rb, Rb(p, xn)82Sr/83Sr, Mo(p, X)90Mo/99Mo, Mo(p, xn)99Tc, 103Rh(p, X)97Ru, 103Rh(p, 4n), (p, 3n), Sb(p, xn)117Te/118Te/119Te, 127I(p, n), (p, 3n), (p, 5n), (p, 6n), 133Cs(p, 6n), (p, 3n), (p, X)129Cs/132Cs, 205Tl(p, 3n), Te(p, xn)205Bi/206Bi, Pb(p, X)201Pb/200Pb, E=5-70 MeV; calculated residuals production σ(E); deduced model, code limitations. ALICE82 code. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0428. 1992LA21 Nucl.Instrum.Methods Phys.Res. B69, 452 (1992) Radionuclide Production with > 70-MeV Proton Accelerators: Current and future prospects NUCLEAR REACTIONS, ICPND 85Rb(p, 4n), (p, 3n), (p, n), 87Rb(p, 6n), (p, 3n)82Sr/83Sr/85Sr, Rb(p, xn)82Sr/83Sr/85Sr, E=threshold-65 MeV; 23Na, Mg, 27Al(p, xnyp), E=threshold-65 MeV; Ne(p, xnyp)18F, E=threshold-67.5 MeV; 23Na, Mg, 27Al(p, xnyp)18F, E=threshold-67.5 MeV; compiled, reviewed residual production σ(E). Other radionuclide production data reviewed.
doi: 10.1016/0168-583X(92)95301-7
1992LA25 Appl.Radiat.Isot. 43, 1005 (1992) M.C.Lagunas-Solar, O.F.Carvacho, P.M.Smith-Jones Cyclotron Production of PET Radionuclides: No-carrier-added fluorine-18 (109.77 min; β + 96.9%; EC 3.1%) with high-energy protons on sodium targets NUCLEAR REACTIONS, ICPND 23Na(p, X)18F, E=20-67.5 MeV; measured residuals yield; deduced σ(E). Model comparison.
doi: 10.1016/0883-2889(92)90219-5
1991LA08 Appl.Radiat.Isot. 42, 643 (1991) M.C.Lagunas-Solar, P.M.Kiefer, O.F.Carvacho, C.A.Lagunas, P.C.Ya Cyclotron Production of NCA 99mTc and 99Mo. An Alternative Non-Reactor Supply Source of Instant 99mTc and 99Mo → 99mTc Generators NUCLEAR REACTIONS, ICPND 100Mo(p, 2n), E=7.6-67.5 MeV; 100Mo(p, np), E=10.6-67.5 MeV; Mo(p, X)90Nb/92Nb/92mNb/87Y/87mY/86Zr/88Zr/89Zr, E < 70 MeV; measured residuals σ(E), cumulative yields.
doi: 10.1016/0883-2889(91)90035-Y
1990LA07 Appl.Radiat.Isot. 41, 521 (1990) M.C.Lagunas-Solar, O.F.Carvacho, S.-T.Yang, Y.Yano Cyclotron Production of PET Radionuclides: 118Sb(3.5 min; β+ 75%; EC 25%) from High-Energy Protons on Natural Sb Targets NUCLEAR REACTIONS, ICPND Sb(p, X)119Te/119mTe/117Te/118Te, E=30-70 MeV; measured residuals production σ(E), single, cumulative yields.
doi: 10.1016/0883-2889(90)90033-D
1988LA01 Appl.Radiat.Isot. 39, 41 (1988) M.C.Lagunas-Solar, O.F.Carvacho, R.R.Cima Cyclotron Production of PET Radionuclides: 18F(109.77 min; β+ 96.9 %; EC 3.1 %) from High-Energy Protons on Metallic Aluminum Targets NUCLEAR REACTIONS, ICPND 27Al(p, n3p), (p, 2n3p), 27Al(p, 2n2α)18F, E=13.3-67.5 MeV; measured thin target, cumulative yields vs E. Activation, radiochemical techniques, 18F residue from 18Ne decay.
doi: 10.1016/0883-2889(88)90090-1
1987LA08 Appl.Radiat.Isot. 38, 129 (1987) M.C.Lagunas-Solar, O.F.Carvacho, L.Nagahara, A.Mishra, N.J.Parks Cyclotron Production of No-Carrier-Added 206Bi (6.24 d) and 205Bi (15.31 d) as Tracers for Biological Studies and for the Development of Alpha-Emitting Radiotherapeutic Agents NUCLEAR REACTIONS, ICPND Pb(p, X)205Bi/206Bi, E=8.8-67.5 MeV; measured σ(Ep), residual yields, total σ. Natural targets, Ge(Li), high-purity Ge detectors.
doi: 10.1016/0883-2889(87)90008-6
1987LA09 Appl.Radiat.Isot. 38, 151 (1987) M.C.Lagunas-Solar, M.J.Avila, P.C.Johnson Targetry and Radiochemical Methods for the Simultaneous Cyclotron Production of No-Carrier-Added Radiopharmaceutical-Quality 100Pd, 97Ru and 101mRh NUCLEAR REACTIONS, ICPND 103Rh(p, X)100Pd/97Ru/101mRh, E=23.3-67.1 MeV; measured residuals thick target yields vs E. Target dissolution, radiochemical method.
doi: 10.1016/0883-2889(87)90013-X
1986LA32 Int.J.Appl.Radiat.Isotop. 37, 823 (1986) M.C.Lagunas-Solar, O.F.Carvacho, Bo-Li Liu, Yutai Jin, Zhao Xiang Sun Cyclotron Production of High-Purity 123I I. A Revision of Excitation Functions, Thin-Target and Cumulative Yields for 127I(p, xn) Reactions NUCLEAR REACTIONS, ICPND 127I(p, n), (p, 3n), (p, 5n), (p, 6n), (p, 7n), E=5.3-67.5 MeV; measured σ(E), thin target residual cumulative yields. Hyperpure Ge detector, multichannel analyzer.
doi: 10.1016/0883-2889(86)90278-9
1986LA33 Int.J.Appl.Radiat.Isotop. 37, 835 (1986) M.C.Lagunas-Solar, O.F.Carvacho, L.J.Harris, C.A.Mathis Cyclotron Production of 122Xe(20.1 h) → 122I(β + 77%; EC 23%; 3.6 min) for Positron Emission Tomography. Current Methods and Potential Developments NUCLEAR REACTIONS, ICPND 127I(p, n), (p, 3n), (p, 5n), (p, 6n), (p, 7n), E=45.8-67.5 MeV; measured σ(E), thin target residual cumulative yields. Hyperpure Ge detector, multichannel analyzer.
doi: 10.1016/0883-2889(86)90279-0
1984JO04 Int.J.Appl.Radiat.Isotop. 35, 371 (1984) P.C.Johnson, M.C.Lagunas-Solar, M.J.Avila The Indirect Production of No-Carrier-Added 57Co via the 59Co(p, 3n)57Ni → 57Co Reaction NUCLEAR REACTIONS, ICPND 59Co(p, 3n)57Ni/57Co, 59Co(p, 3np), E=10-40 MeV; measured residual, β--decay daughter thick target, cumulative yields vs E, production σ(E), reaction σ(E).
doi: 10.1016/0020-708X(84)90044-9
1984LA23 Int.J.Appl.Radiat.Isotop. 35, 743 (1984) M.C.Lagunas-Solar, M.J.Avila, P.C.Johnson Cyclotron Production of 101mRh via Proton-Induced Reactions on 103Rh Targets NUCLEAR REACTIONS, ICPND 103Rh(p, 2np), (p, nd), (p, t), (p, 3n), (p, 3np), (p, 2nd), (p, nt), (p, 4n), E=15-67 MeV; measured thin target residual yields, 100,101Pd, 101m,101,100Rh production σ(E). Avtivation technique.
doi: 10.1016/0020-708X(84)90080-2
1983LA15 Int.J.Appl.Radiat.Isotop. 34, 915 (1983) M.C.Lagunas-Solar, M.J.Avila, N.J.Navarro, P.C.Johnson Cyclotron Production of No-Carrier-Added 97Ru by Proton Bombardment of 103Rh Targets NUCLEAR REACTIONS, ICPND 103Rh(p, xn), (p, xnyp), (p, xnypzd), (p, xnyd), (p, xnypzt), (p, xnydzt), (p, xnyt), (p, xnyα), (p, 2n5He), (p, n6He)97Ru, E=37.5-67.5 MeV; measured residual nucleus cummulative, thick target yields, σ vs E. Radiochemical methods.
doi: 10.1016/0020-708X(83)90154-0
1983LI09 Int.J.Appl.Radiat.Isotop. 34, 631 (1983) Cyclotron Production of 67Ga. Cross Sections and Thick-Target Yields for the 67Zn(p, n) and 68Zn(p, 2n) Reactions NUCLEAR REACTIONS, ICPND 66,67Zn(p, n)67Ga, 67Zn(p, 2n), 68Zn(p, 2n)67Ga, 68Zn(p, 3n), E ≥ 35 MeV; measured residuals yields vs E, reaction σ, production σ for 67Ga.
doi: 10.1016/0020-708X(83)90067-4
1982LA15 Int.J.Appl.Radiat.Isotop. 33, 619 (1982) M.C.Lagunas-Solar, F.E.Little, H.A.Moore, Jr. Cyclotron Production of 128Cs (3.62 min). A New Positron-Emitting Radionuclide for Medical Applications RADIOACTIVITY 128Ba(EC), 129mBa(EC), (β+), 129Ba(EC), (β+), 131Ba(EC) [from 133Cs(p, xnyp), E=36.4-67 MeV]; 128Cs [from 128Ba decay]; measured Eγ, Iγ. CsCl target, elution technique. NUCLEAR REACTIONS, ICPND 133Cs(p, np), (p, 3n), (p, 6n), (p, 5n)129Cs/128Cs, E=36.4-67 MeV; measured residuals production σ, thick target, cumulative yields vs E. CsCl target.
doi: 10.1016/0020-708X(82)90059-X
1982LA23 J.Labelled Compd.Radiopharm. 19, 1436 (1982) M.C.Lagunas-Solar, M.J.Avila, N.J.Navarro, P.C.Johnson Cyclotron Production of Ruthenium-97 (NCA) with 67.5 MeV Protons on Rhodium Targets NUCLEAR REACTIONS, ICPND 103Rh(p, 7n), (p, 6np), (p, 5n2p), (p, 3n2d), (p, 4n3He), (p, 3npt), (p, 2ndt), (p, n2t), (p, 3nα), E=37.8-67.1 MeV; measured residuals thick target, cumulative yields, total σ vs E. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0194. 1980LA14 Int.J.Appl.Radiat.Isotop. 31, 117 (1980) M.C.Lagunas-Solar, J.A.Jungerman, D.W.Paulson Thallium-201 Yeilds and Excitation Functions for the Lead Radioactivities Produced by Irradiation of Thallium-205 with 34-60 MeV Protons RADIOACTIVITY 201Pb [from 205Tl(p, xn), E=34-60 MeV]; measured Eγ, T1/2. 201Tl deduced yield. NUCLEAR REACTIONS 205Tl(p, xn), E=34-60 MeV; measured production σ(E) for 200,201.202,203,204Pb.
doi: 10.1016/0020-708X(80)90054-X
1979LA19 Int.J.Appl.Radiat.Isotop. 30, 25 (1979) M.C.Lagunas-Solar, J.A.Jungerman Cyclotron Production of Carrier-Free Cobalt-55, a New Positron-Emitting Label for Bleomycin RADIOACTIVITY 55Co; measured T1/2. NUCLEAR REACTIONS 56Fe(p, xn), E=15-40 MeV; measured production σ(E) for 55Co, 52Mn, 56Co. Thin, thick natural Fe targets.
doi: 10.1016/0020-708X(79)90093-0
1978LA20 Int.J.Appl.Radiat.Isotop. 29, 159 (1978) M.C.Lagunas-Solar, J.A.Jungerman, N.F.Peek, R.M.Theus Thallium-201 Yields and Excitation Functions for the Lead Radioactivities Produced by Irradiation of Natural Thallium with 15-60 MeV Protons NUCLEAR REACTIONS Tl(p, xn), (p, xnyp), E=15-60 MeV; measured production σ of 200,201,202m,203,204mPb, 201Tl. Chemical separation.
doi: 10.1016/0020-708X(78)90138-2
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