NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = O.F.Carvacho Found 8 matches. 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
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
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
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