2015
DOI: 10.1016/j.apradiso.2015.06.022
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Nuclear model calculation and targetry recipe for production of 110mIn

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Cited by 6 publications
(3 citation statements)
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“…The most promising methods for direct production of 110m In include 110 Cd­(p,n), 107 Ag­(α,n), and 109 Ag­( 3 He,2n); however, coproduction of 110g In ( t 1/2 = 4.9 h) tends to dilute isotopic purity and remains problematic . For example, following yield-optimizing calculations, Kakavand et al irradiated nat Cd with 15 MeV protons (100 μA, 1 h) and produced 44.3 ± 8.8 GBq/C (gigabecquerel per Coulomb) with 1.25 ± 0.25 GBq/C 110g In impurity. , Indirect production using 110 Sn ( t 1/2 = 4.11 h, EC 100%) as a parent radionuclide can yield 110g In-free 110m In following electron capture and is achieved via 113 In­(p,4n), 113 In­(d,5n), 110 Cd­( 3 He,3n), 108 Cd­(α,2n), or 110 Cd­(α,4n). , To make future use viable, production of 111/113 In must be mitigated through the use of enriched targets and beam energy optimization . A clinical proof-of-concept study with 110m In-DTPA- d -Phe-octreotide was conducted in 2002 to demonstrate the superiority of 110m In PET compared to 111 In SPECT.…”
Section: Indiummentioning
confidence: 99%
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“…The most promising methods for direct production of 110m In include 110 Cd­(p,n), 107 Ag­(α,n), and 109 Ag­( 3 He,2n); however, coproduction of 110g In ( t 1/2 = 4.9 h) tends to dilute isotopic purity and remains problematic . For example, following yield-optimizing calculations, Kakavand et al irradiated nat Cd with 15 MeV protons (100 μA, 1 h) and produced 44.3 ± 8.8 GBq/C (gigabecquerel per Coulomb) with 1.25 ± 0.25 GBq/C 110g In impurity. , Indirect production using 110 Sn ( t 1/2 = 4.11 h, EC 100%) as a parent radionuclide can yield 110g In-free 110m In following electron capture and is achieved via 113 In­(p,4n), 113 In­(d,5n), 110 Cd­( 3 He,3n), 108 Cd­(α,2n), or 110 Cd­(α,4n). , To make future use viable, production of 111/113 In must be mitigated through the use of enriched targets and beam energy optimization . A clinical proof-of-concept study with 110m In-DTPA- d -Phe-octreotide was conducted in 2002 to demonstrate the superiority of 110m In PET compared to 111 In SPECT.…”
Section: Indiummentioning
confidence: 99%
“…401 For example, following yield-optimizing calculations, Kakavand et al irradiated nat Cd with 15 MeV protons (100 μA, 1 h) and produced 44.3 ± 8.8 GBq/C (gigabecquerel per Coulomb) with 1.25 ± 0.25 GBq/C 110g In impurity. 402,403 Indirect production using 110 Sn (t 1/2 = 4.11 h, EC 100%) as a parent radionuclide can yield 110g In-free 110m In following electron capture and is achieved via 113 In(p,4n), 113 In(d,5n), 110 Cd-( 3 He,3n), 108 Cd(α,2n), or 110 Cd(α,4n). 401,404−406 To make future use viable, production of 111/113 In must be mitigated through the use of enriched targets and beam energy optimization.…”
Section: Indium-110m Productionmentioning
confidence: 99%
“…The direct production of 110m In (J π = 2 + ) always leads to the co-formation of the radioactive impurity 110g In (J π = 7 + ) but the higher isomeric ratio can be achieved with lower projectile energies. The recommended reaction, 110 Cd(p,n) (Otozai et al, 1966;Abramovich et al, 1975;Skakun et al, 1975;Kormali et al, 1976;Marten et al, 1985;Nortier et al, 1990;Tárkányi et al, 11/38 2006Tárkányi et al, 11/38 , 2015Al-Saleh, 2008;Khandaker et al, 2008;Büyükuslu et al, 2010), at 15 MeV energy (available in the commonly used machines) and with electroplated nat Cd target (Kakavand et al, 2015b) yields 160 MBq/uAh of 110m In with reported 3% of 110g In and 6% of 111g In radioactive impurities (Mukhammedov et al, 1984;Kakavand et al, 2015b).…”
Section: M Tcmentioning
confidence: 99%