ENTRY A0445 20220804 A102A044500000001 SUBENT A0445001 20220804 A102A044500100001 BIB 11 42 A044500100002 TITLE Cyclotron production of PET radionuclides- A044500100003 F-18 (109.77 min, beta+ 96.9%, EC 3.1%) A044500100004 from high-energy protons on metallic aluminum targets A044500100005 AUTHOR (M.C.Lagunas-Solar,O.F.Carvacho,R.R.Cima) A044500100006 INSTITUTE (1USADAV) A044500100007 REFERENCE (J,ARI,39,41,1988) A044500100008 SAMPLE Metallic aluminum was used for the fabrication of A044500100009 thin targets (0.085 cm,2.54-cm outer diam.,0.23 g/cm2).A044500100010 FACILITY (ISOCY,1USADAV) A044500100011 METHOD (EXTB,STTA,ACTIV,CHSEP,BCINT) A044500100012 DETECTOR (HPGE) A044500100013 ADD-RES (TTY-C) Thin and thick targets yields have been A044500100014 measured. A044500100015 ERR-ANALYS (EN-ERR,1.4,29.) The total uncertainty in energy A044500100016 calculation range from 1.4% at 67 MeV to 29% at 7. MeV.A044500100017 This uncertainty includes: A044500100018 * The error in the incident beam energy - 1% A044500100019 * The error in the range values - 1% A044500100020 * The error in the Al-target density - 0.1% A044500100021 * The error in the Al-target thickness (weighing A044500100022 errors) - 0.1% A044500100023 The excitation functions reported here have energy A044500100024 uncertainties ranging from +-1. MeV at 67.5 MeV, A044500100025 to +-2. MeV at 7. MeV. A044500100026 (ERR-T) The total uncertainty in the cross section A044500100027 and radionuclide-yield values was calculated as 9%. A044500100028 The total uncertainty includes: A044500100029 (ERR-2) The uncertainty in the beam-current integrationA044500100030 (ERR-3) The uncertainty in the calibration sources A044500100031 (ERR-4) The uncertainty in the detector efficiency A044500100032 (ERR-5) The uncertainty in the counting geometry. A044500100033 (ERR-6) The uncertainty in the decay corrections. A044500100034 (ERR-7) The uncertainty in the gamma-ray abundances A044500100035 (ERR-8) The uncertainty in the integration A044500100036 routines(average) is 3% (the maximum uncertainty in A044500100037 the integration routines is 10%). A044500100038 HISTORY (19910228C) A044500100039 (19920608U) A044500100040 (19920203A) According to memo CP-D/223. A044500100041 (20220804A) SD:Updated to new date formats, lower case.A044500100042 Corrections in all Subents. Subent 003 was split in A044500100043 two (Subent 004 added). A044500100044 ENDBIB 42 0 A044500100045 COMMON 8 6 A044500100046 ERR-2 ERR-3 ERR-4 ERR-5 ERR-6 ERR-7 A044500100047 ERR-8 ERR-T A044500100048 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A044500100049 PER-CENT PER-CENT A044500100050 3. 3. 5. 1. 2. 5. A044500100051 3. 9. A044500100052 ENDCOMMON 6 0 A044500100053 ENDSUBENT 52 0 A044500199999 SUBENT A0445002 20220804 A102A044500200001 BIB 4 4 A044500200002 REACTION (13-AL-27(P,X)9-F-18,,SIG) A044500200003 DECAY-DATA (9-F-18,109.77MIN,DG) A044500200004 STATUS (TABLE) Tbl.2 from Appl.Radiat.Isot.,39(1988)41 A044500200005 HISTORY (20220804A) SD: SF9=EXP deleted from REACTION code. A044500200006 ENDBIB 4 0 A044500200007 NOCOMMON 0 0 A044500200008 DATA 2 19 A044500200009 EN DATA A044500200010 MEV MB A044500200011 66.6 7.5 A044500200012 64.8 7.7 A044500200013 63.0 8.3 A044500200014 61.1 7.6 A044500200015 59.2 7.5 A044500200016 57.2 7.0 A044500200017 55.2 6.7 A044500200018 53.2 5.5 A044500200019 51.0 4.6 A044500200020 48.9 3.1 A044500200021 46.8 2.0 A044500200022 44.5 1.1 A044500200023 42.1 0.7 A044500200024 39.5 0.3 A044500200025 36.8 0.2 A044500200026 34.0 0.2 A044500200027 31.1 0.1 A044500200028 27.9 0.1 A044500200029 24.3 0.1 A044500200030 ENDDATA 21 0 A044500200031 ENDSUBENT 30 0 A044500299999 SUBENT A0445003 20220804 A102A044500300001 BIB 4 6 A044500300002 REACTION (13-AL-27(P,X)11-NA-24,,SIG) A044500300003 REL-REF (A,B0082002,R.Holub+,J,NP/A,288,291,1977) A044500300004 (A,A0178019,A.Grutter+,J,NP/A,383,98,1982) A044500300005 STATUS (TABLE) Tbl.3 from Appl.Radiat.Isot.,39(1988)41 A044500300006 HISTORY (20220804A) SD: SF9=EXP deleted from REACTION code. A044500300007 Subent was split (see Subent 004). A044500300008 ENDBIB 6 0 A044500300009 NOCOMMON 0 0 A044500300010 DATA 2 22 A044500300011 EN DATA A044500300012 MEV MB A044500300013 66.6 9.3 A044500300014 64.8 8.9 A044500300015 63.0 8.3 A044500300016 61.1 8.5 A044500300017 59.2 8.2 A044500300018 57.2 7.8 A044500300019 55.2 7.4 A044500300020 53.2 6.7 A044500300021 51.0 5.6 A044500300022 48.9 4.6 A044500300023 46.8 3.7 A044500300024 44.5 2.7 A044500300025 42.1 2.2 A044500300026 39.5 1.6 A044500300027 36.8 0.9 A044500300028 34.0 0.7 A044500300029 31.1 0.5 A044500300030 27.9 0.4 A044500300031 24.3 0.4 A044500300032 20.3 0.3 A044500300033 15.8 0.2 A044500300034 10.2 0.2 A044500300035 ENDDATA 24 0 A044500300036 ENDSUBENT 35 0 A044500399999 SUBENT A0445004 20220804 A102A044500400001 BIB 4 5 A044500400002 REACTION (13-AL-27(P,X)11-NA-22,,SIG) A044500400003 REL-REF (A,B0082002,R.Holub+,J,NP/A,288,291,1977) A044500400004 (A,A0178019,A.Grutter+,J,NP/A,383,98,1982) A044500400005 STATUS (TABLE) Tbl.3 from Appl.Radiat.Isot.,39(1988)41 A044500400006 HISTORY (20220804T) SD: Part of Subent 003. A044500400007 ENDBIB 5 0 A044500400008 NOCOMMON 0 0 A044500400009 DATA 2 18 A044500400010 EN DATA A044500400011 MEV MB A044500400012 66.6 24.6 A044500400013 64.8 21.5 A044500400014 63.0 24.3 A044500400015 61.1 25.1 A044500400016 59.2 26.1 A044500400017 57.2 27.6 A044500400018 55.2 29.8 A044500400019 53.2 32.2 A044500400020 51.0 34.7 A044500400021 48.9 38.0 A044500400022 46.8 40.4 A044500400023 44.5 42.6 A044500400024 42.1 40.5 A044500400025 39.5 35.1 A044500400026 36.8 25.5 A044500400027 34.0 13.0 A044500400028 31.1 3.2 A044500400029 27.9 0.2 A044500400030 ENDDATA 20 0 A044500400031 ENDSUBENT 30 0 A044500499999 ENDENTRY 4 0 A044599999999