Abstract:The low intensity fl+/E.C, branches in the decay of 45Ti to excited states of 45Sc have been reinvestigated in order to resolve discrepancies in reported branching ratios. A new branch to the 974 keV level, having an intensity of 9.9_+ 1.2 • 10-5/decay has been found. A previously reported branch to the 1237 keV level was found to be in error. The intensities for decay to the levels at 720, 1408 and 1661 keV levels were determined to be 154+ 12, 90.2_+9.7 and 52.5_+ 5.6, respectively, in units of 10 -5 per dec… Show more
“…Porter et al [22] and Zuk et al [23] is (84.80 ± 0.13)% and is based on theoretical values of Zweifel [31]. However, this result had not been experimentally confirmed up to now.…”
Section: Discussionmentioning
confidence: 84%
“…The intensities of the -rays 1237.07, 1408.6 and 1662.4 keV were found to be smaller as was expected, having values of (0.0161 ± 0.005)%, (0.0696 ± 0.0067)% and (0.00299 ± 0.0039)%, respectively. The comparison of these data with the -ray intensities shown in Table 2, published by the three research groups mentioned above [21][22][23] To evaluate these different data sets, the earlier works have to be examined in detail. All three older studies show at least a few drawbacks in their experimental set-up.…”
Section: Discussionmentioning
confidence: 99%
“…In 1965 Gföller and Flammersfeld [21] determined the four most intense -rays connected with its decay. Porter et al [22] re-measured the values in 1966, followed by Zuk et al [23] in the early 1970's whose results are considered as standard till today. However, due to limited or unknown sample purity and fragmentary measurement protocols, the reliability of the data of all three studies remains unclear.…”
Abstract:To evaluate the PET-imaging properties of the promising positron emitter 45 Ti, its + -and -ray intensities were measured. Use of the cation-exchange resin DOWEX 50W×8 (H + -form) enabled the isolation of radiochemically pure, no-carrier-added 45 Ti from "bulk" scandium after proton bombardment. Thin, no-carrier-added 45 Ti samples were prepared. The combination of -ray and X-ray spectrometry with -coincidence counting allowed for the first time the experimental determination of the positron intensity as (85.67 ± 2.23)% and the absolute intensity of the 720.22 keV -ray as (0.1171 ± 0.0057)%.
“…Porter et al [22] and Zuk et al [23] is (84.80 ± 0.13)% and is based on theoretical values of Zweifel [31]. However, this result had not been experimentally confirmed up to now.…”
Section: Discussionmentioning
confidence: 84%
“…The intensities of the -rays 1237.07, 1408.6 and 1662.4 keV were found to be smaller as was expected, having values of (0.0161 ± 0.005)%, (0.0696 ± 0.0067)% and (0.00299 ± 0.0039)%, respectively. The comparison of these data with the -ray intensities shown in Table 2, published by the three research groups mentioned above [21][22][23] To evaluate these different data sets, the earlier works have to be examined in detail. All three older studies show at least a few drawbacks in their experimental set-up.…”
Section: Discussionmentioning
confidence: 99%
“…In 1965 Gföller and Flammersfeld [21] determined the four most intense -rays connected with its decay. Porter et al [22] re-measured the values in 1966, followed by Zuk et al [23] in the early 1970's whose results are considered as standard till today. However, due to limited or unknown sample purity and fragmentary measurement protocols, the reliability of the data of all three studies remains unclear.…”
Abstract:To evaluate the PET-imaging properties of the promising positron emitter 45 Ti, its + -and -ray intensities were measured. Use of the cation-exchange resin DOWEX 50W×8 (H + -form) enabled the isolation of radiochemically pure, no-carrier-added 45 Ti from "bulk" scandium after proton bombardment. Thin, no-carrier-added 45 Ti samples were prepared. The combination of -ray and X-ray spectrometry with -coincidence counting allowed for the first time the experimental determination of the positron intensity as (85.67 ± 2.23)% and the absolute intensity of the 720.22 keV -ray as (0.1171 ± 0.0057)%.
“…Titanium radionuclides were first synthesized over 80 years ago 2 and are currently being revived due to their promising characteristics in nuclear medicine, especially for positron emission tomography (PET) imaging. 3–7 From a cyclotron, two types of Ti isotopes can be produced: a long-lived titanium-44 ( 44 Ti: t 1/2 = 60 years) 8 which is not-well suited for direct PET applications, and titanium-45 ( 45 Ti: t 1/2 = 3.08 h, β + : 84.8%, E β+avg = 439 keV) 3 with negligible secondary γ-emission (0.154%) and a low β + maximum endpoint energy of 1040.4 keV, which are favourable features for ensuring good image quality at low dosing for PET imaging.…”
We report the first use of 1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetic acid (DOTA) as a chelator for titanium. The resulting complex is fully characterised and extended to the radiolabelling of DOTA with titanium-45.
“…The energy levels and their decay properties have been investigated by many authors. When this work was begun the information available on the 45SC nucleus had been obtained from the following experiments : Coulomb excitation [3][4][5][6][7][8][9][10], beta-decay [9], [11,12], radiative proton capture [13][14][15][16], inelastic proton scattering [10], [17][18][19][20][21], one or two particle transfer reactions [22][23][24][25] and the (a, py) reaction [26,27]. The low-lying negative parity states from I' = 1/2to 15/2-have been extensively discussed in all these papers.…”
The electromagnetic decays of the negative parity states in 45Sc up to an excitation energy of 2107 keV have been investigated via the 42Ca(α, pγ)45Sc reaction at a bombarding energy of 10.5 MeV. Reaction produced protons were detected in an annular silicon detector at an average angle of 171°. Gamma-ray spectra were measured with a Ge(Li) detector at angles 105° ≥ θ ≥ 0°. Spins and lifetimes of the levels as well as branching and mixing ratios of their decay γ-rays have been obtained from proton-gamma angular correlation measurements. Reduced electromagnetic transition matrix elements have been extracted for a number of observed transitions. Calculations based on the strong coupling model have been performed. The results are compared with experiment
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