Pub Date : 1985-09-01DOI: 10.1016/0020-708X(85)90042-0
M. Van der Leij, B.W. Van Halteren, G.A. Brinkman
Cross sections per equivalent quantum (σq) have been measured for photonuclear reactions yielding 18F from LiF, SF6, CF4, Ne and metallic Na targets, in the energy range 77–125 MeV. The σq values for LiF and Na are conformable with known data, whilst the σq values for SF6 and CF4 are found to be 10% lower than for LiF. The utility of metallic Na as a target for 18F production has been demostrated by a nucleophilic substitution reaction with (C2H5)4N18F, formed after dissolution of irradiated Na in absolute C2H5OH.
{"title":"Photonuclear production of 18F from F, Ne and (metallic) Na","authors":"M. Van der Leij, B.W. Van Halteren, G.A. Brinkman","doi":"10.1016/0020-708X(85)90042-0","DOIUrl":"10.1016/0020-708X(85)90042-0","url":null,"abstract":"<div><p>Cross sections per equivalent quantum (σ<sub>q</sub>) have been measured for photonuclear reactions yielding <sup>18</sup>F from LiF, SF<sub>6</sub>, CF<sub>4</sub>, Ne and metallic Na targets, in the energy range 77–125 MeV. The σ<sub>q</sub> values for LiF and Na are conformable with known data, whilst the σ<sub>q</sub> values for SF<sub>6</sub> and CF<sub>4</sub> are found to be 10% lower than for LiF. The utility of metallic Na as a target for <sup>18</sup>F production has been demostrated by a nucleophilic substitution reaction with (C<sub>2</sub>H<sub>5</sub>)<sub>4</sub>N<sup>18</sup>F, formed after dissolution of irradiated Na in absolute C<sub>2</sub>H<sub>5</sub>OH.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 9","pages":"Pages 717-719"},"PeriodicalIF":0.0,"publicationDate":"1985-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90042-0","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"73772199","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-09-01DOI: 10.1016/0020-708X(85)90039-0
Cihan Özmutlu
Scattering of 59.6 keV γ-rays of 241Am from sodium iodide, aluminium and copper have been determined for scattering angles between 24 and 144°. Differential coherent plus incoherent scattering cross section values for copper have been obtained theoretically, by means of form factor and scattering function calculations. Comparing the experimental data with the theoretical cross section values for copper, the experimental arrangement has been calibrated for each scattering angle. So, absolute values of differential cross section of sodium iodide for 59.6 keV γ-rays for eleven scattering angles have been obtained.
{"title":"Measurement of differential scattering cross section of NaI for 59.6 keV gamma rays","authors":"Cihan Özmutlu","doi":"10.1016/0020-708X(85)90039-0","DOIUrl":"10.1016/0020-708X(85)90039-0","url":null,"abstract":"<div><p>Scattering of 59.6 keV γ-rays of <sup>241</sup>Am from sodium iodide, aluminium and copper have been determined for scattering angles between 24 and 144°. Differential coherent plus incoherent scattering cross section values for copper have been obtained theoretically, by means of form factor and scattering function calculations. Comparing the experimental data with the theoretical cross section values for copper, the experimental arrangement has been calibrated for each scattering angle. So, absolute values of differential cross section of sodium iodide for 59.6 keV γ-rays for eleven scattering angles have been obtained.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 9","pages":"Pages 699-703"},"PeriodicalIF":0.0,"publicationDate":"1985-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90039-0","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"77845769","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-09-01DOI: 10.1016/0020-708X(85)90043-2
David W. Anderson , Karl L. Prado
A clinical electron linear accelerator was adapted for continuous energy selection and used to measure bremsstrahlung yield for the photonuclear reaction 27Al (γ, 2p) 25Na from 24.0 to 32.0-MeV in 0.25 MeV steps. A germanium detector was used to measure the number of photoproduct γ-rays emitted. The yield values were analyzed for photonuclear cross section using PHONUC II, a program especially adapted for use with yield data from thick-target bremsstrahlung. The cross section shows distinct resonance peaks at 26.3±0.3, 27.3±0.4 and 30.3±0.5 MeV. Possible theoretical origins of these resonances and applications of the reaction in accelerator energy calibration are discussed.
{"title":"Measurement of yield and cross section for the 27Al (γ, 2p) 25Na reaction with a clinical linear accelerator","authors":"David W. Anderson , Karl L. Prado","doi":"10.1016/0020-708X(85)90043-2","DOIUrl":"10.1016/0020-708X(85)90043-2","url":null,"abstract":"<div><p>A clinical electron linear accelerator was adapted for continuous energy selection and used to measure bremsstrahlung yield for the photonuclear reaction <sup>27</sup>Al (γ, 2p) <sup>25</sup>Na from 24.0 to 32.0-MeV in 0.25 MeV steps. A germanium detector was used to measure the number of photoproduct γ-rays emitted. The yield values were analyzed for photonuclear cross section using PHONUC II, a program especially adapted for use with yield data from thick-target bremsstrahlung. The cross section shows distinct resonance peaks at 26.3±0.3, 27.3±0.4 and 30.3±0.5 MeV. Possible theoretical origins of these resonances and applications of the reaction in accelerator energy calibration are discussed.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 9","pages":"Pages 721-725"},"PeriodicalIF":0.0,"publicationDate":"1985-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90043-2","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"15177410","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-09-01DOI: 10.1016/0020-708X(85)90049-3
Roger F. Martin, Marshall Pardee
The DNA ligand Hoechst 33258 has been iodinated with carrier-free [125I]iodide by the lactoperoxidase method. The product was separated from other iodination products and the uniodinated compound by preparative thin layer chromatography. 125I-labelled Hoechst 33258 is useful as a probe with DNA molecules of defined sequence since the decay of the 125I atom results in the induction of a double-strand break, the location of which can be detected by DNA-sequencing techniques.
{"title":"Preparation of carrier free [125I]IodoHoechst 33258","authors":"Roger F. Martin, Marshall Pardee","doi":"10.1016/0020-708X(85)90049-3","DOIUrl":"10.1016/0020-708X(85)90049-3","url":null,"abstract":"<div><p>The DNA ligand Hoechst 33258 has been iodinated with carrier-free [<sup>125</sup>I]iodide by the lactoperoxidase method. The product was separated from other iodination products and the uniodinated compound by preparative thin layer chromatography. <sup>125</sup>I-labelled Hoechst 33258 is useful as a probe with DNA molecules of defined sequence since the decay of the <sup>125</sup>I atom results in the induction of a double-strand break, the location of which can be detected by DNA-sequencing techniques.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 9","pages":"Pages 745-747"},"PeriodicalIF":0.0,"publicationDate":"1985-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90049-3","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"13564174","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-08-01DOI: 10.1016/0020-708X(85)90009-2
Janis Gulens , William J. Olmstead , Arthur S. Denovan , Kathleen L. Gale , John H. Rolston
The oxygen isotopic content of natural and heavy water has been determined by mass spectrometric analysis of oxygen gas, produced by direct chemical oxidation using either Na2S2O8 in strongly basic media or ClF3. The results from the two methods are in good agreement. No evidence for mass independent isotope fractionation effects in deuterium-free water or in heavy water samples from a variety of sources was found. The 17O and 18O content of three IAEA water standards (V-SMOW, GISP and SLAP) are reported.
{"title":"Determination of oxygen isotopes in water by direct oxidation and oxygen mass spectrometry","authors":"Janis Gulens , William J. Olmstead , Arthur S. Denovan , Kathleen L. Gale , John H. Rolston","doi":"10.1016/0020-708X(85)90009-2","DOIUrl":"10.1016/0020-708X(85)90009-2","url":null,"abstract":"<div><p>The oxygen isotopic content of natural and heavy water has been determined by mass spectrometric analysis of oxygen gas, produced by direct chemical oxidation using either Na<sub>2</sub>S<sub>2</sub>O<sub>8</sub> in strongly basic media or ClF<sub>3</sub>. The results from the two methods are in good agreement. No evidence for mass independent isotope fractionation effects in deuterium-free water or in heavy water samples from a variety of sources was found. The <sup>17</sup>O and <sup>18</sup>O content of three IAEA water standards (V-SMOW, GISP and SLAP) are reported.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 8","pages":"Pages 663-667"},"PeriodicalIF":0.0,"publicationDate":"1985-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90009-2","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89145070","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-08-01DOI: 10.1016/0020-708X(85)90008-0
Petr Kopecký
Cross sections for the Cu(p, x) 58Co, 63Cu(p, 2n) 62Zn and 65Cu(p, n) 65Zn reactions were measured in the energy region from 4 to 33 MeV. The excitation functions for 58Co, 62Zn and 65Zn were determined and compared with the published data. The experimental cross sections have been used as reference data for proton beam monitoring in the energy range of 13–33 MeV.
{"title":"Proton beam monitoring via the Cu(p, x) 58Co, 63Cu(p, 2n) 62Zn and 65Cu(p, n) 65Zn reactions in copper","authors":"Petr Kopecký","doi":"10.1016/0020-708X(85)90008-0","DOIUrl":"10.1016/0020-708X(85)90008-0","url":null,"abstract":"<div><p>Cross sections for the Cu(p, x) <sup>58</sup>Co, <sup>63</sup>Cu(p, 2n) <sup>62</sup>Zn and <sup>65</sup>Cu(p, n) <sup>65</sup>Zn reactions were measured in the energy region from 4 to 33 MeV. The excitation functions for <sup>58</sup>Co, <sup>62</sup>Zn and <sup>65</sup>Zn were determined and compared with the published data. The experimental cross sections have been used as reference data for proton beam monitoring in the energy range of 13–33 MeV.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 8","pages":"Pages 657-661"},"PeriodicalIF":0.0,"publicationDate":"1985-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90008-0","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79859289","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-08-01DOI: 10.1016/0020-708X(85)90005-5
Mirko Diksic, Pasquale Diraddo
This paper describes a convenient, high-yield synthesis of [18F]4-fluoroantipyrine, a blood flow tracer, by fluorination of antipyrine with [18F]acetylhypofluorite prepared in situ. The radiopharmaceutical was obtained in a radiochemical yield of 28 and 30% following HPLC and Sep-Pak purification, respectively. The two different purification procedures of the crude reaction are described. Sep-Pak filtration, after decomposition of the intermediary of the fluorination reaction by heating with NaOCH3 in CH3CN, produced a radiopharmaceutical with radiochemical purity of more than 98%. The synthesis requires 50 min following irradiation.
{"title":"A convenient, high-yield synthesis of [18F]4-fluoroantipyrine using [18F]acetylhypofluorite","authors":"Mirko Diksic, Pasquale Diraddo","doi":"10.1016/0020-708X(85)90005-5","DOIUrl":"10.1016/0020-708X(85)90005-5","url":null,"abstract":"<div><p>This paper describes a convenient, high-yield synthesis of [<sup>18</sup>F]4-fluoroantipyrine, a blood flow tracer, by fluorination of antipyrine with [<sup>18</sup>F]acetylhypofluorite prepared <em>in situ</em>. The radiopharmaceutical was obtained in a radiochemical yield of 28 and 30% following HPLC and Sep-Pak purification, respectively. The two different purification procedures of the crude reaction are described. Sep-Pak filtration, after decomposition of the intermediary of the fluorination reaction by heating with NaOCH<sub>3</sub> in CH<sub>3</sub>CN, produced a radiopharmaceutical with radiochemical purity of more than 98%. The synthesis requires 50 min following irradiation.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 8","pages":"Pages 643-645"},"PeriodicalIF":0.0,"publicationDate":"1985-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90005-5","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"83734526","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-08-01DOI: 10.1016/0020-708X(85)90003-1
M.J. Millen, B.D. Sowerby
The ash content of coal can be determined by a technique based on pair production (PP). The PP technique has been previously proved in the laboratory and in the field, and five commercial PP gauges are in routine use at coal washeries in Australia. However for some applications on coals of highly variable ash composition, there is a need for improved accuracy.
Calculations and experiments have been made to investigate two methods of improving PP gauge accuracy for coals with highly variable ash composition. The first combines the PP gauge measurement with measurements of the low-energy part of the PP gauge spectrum and the second is done in conjunction with separate low and high energy γ-ray transmission measurements. Calculations show that these methods can correct the PP gauge assay exactly when the concentration of a single high-Z element in the ash varies. When more than one element varies, the error reduction is less and depends on the elements and their variations. Experiments with a group of samples from Blackwater, Queensland showed that gauge accuracy improved by about 20% relative using the first method. Use of the second method on two groups of samples from Blackwater and South Africa produced about 15% improvement. There was no reduction in error when either method was used on a third group of samples from the Hunter Valley, New South Wales.
{"title":"Correction of pair production gauge ash determinations for changes in coal ash composition","authors":"M.J. Millen, B.D. Sowerby","doi":"10.1016/0020-708X(85)90003-1","DOIUrl":"10.1016/0020-708X(85)90003-1","url":null,"abstract":"<div><p>The ash content of coal can be determined by a technique based on pair production (PP). The PP technique has been previously proved in the laboratory and in the field, and five commercial PP gauges are in routine use at coal washeries in Australia. However for some applications on coals of highly variable ash composition, there is a need for improved accuracy.</p><p>Calculations and experiments have been made to investigate two methods of improving PP gauge accuracy for coals with highly variable ash composition. The first combines the PP gauge measurement with measurements of the low-energy part of the PP gauge spectrum and the second is done in conjunction with separate low and high energy γ-ray transmission measurements. Calculations show that these methods can correct the PP gauge assay exactly when the concentration of a single high-Z element in the ash varies. When more than one element varies, the error reduction is less and depends on the elements and their variations. Experiments with a group of samples from Blackwater, Queensland showed that gauge accuracy improved by about 20% relative using the first method. Use of the second method on two groups of samples from Blackwater and South Africa produced about 15% improvement. There was no reduction in error when either method was used on a third group of samples from the Hunter Valley, New South Wales.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 8","pages":"Pages 627-633"},"PeriodicalIF":0.0,"publicationDate":"1985-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90003-1","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84261783","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-08-01DOI: 10.1016/0020-708X(85)90004-3
Z. Kovács , G. Blessing, S.M. Qaim, G. Stöcklin
Excitation functions were measured by the stacked-foil technique for the reactions 76Se(p, n)76Br, 76Se(p, 2n)75Br, 76Se(p, 3n)74mBr, 76Se(p, α)73As, 76Se(p, αn)72As, 76Se(p, α2n)71As and 76Se(p, 3He + 2pn + pd)74As on 96.48% enriched 76Se up to Ep = 40 MeV. The optimum energy range for the production of 75Br via the 76Se(p, 2n)75Br reaction at our compact cyclotron is Ep = 24 → 21.5 MeV, the calculated thick target yield of 75Br amounting to 32 mCi/μ Ah and the expected level of 76Br-impurity to 2.0%. A thin layer of metallic 76Se on Al-backing was used as target in combination with a water-cooled rotating target head. A dry distillation technique for the separation of radiobromine from irradiated targets was developed; radiochemical yields of about 40–52% were obtained. Using a 50.2 mg/cm2 thick target (Ep = 24→21.85 MeV, an irradiation time of 1.25 h at a nominal proton beam current of 15 μA and a distillation time of 30 min at 300°C, about 160 mCi of 75Br (at EOB) is produced. The total loss of 76Se after irradiation and distillation process is <1%. The levels of 76Br and 77Br impurities in 75Br are <3% and 0.15%, respectively.
{"title":"Production of 75Br via the 76Se(p, 2n)75Br reaction at a compact cyclotron","authors":"Z. Kovács , G. Blessing, S.M. Qaim, G. Stöcklin","doi":"10.1016/0020-708X(85)90004-3","DOIUrl":"10.1016/0020-708X(85)90004-3","url":null,"abstract":"<div><p>Excitation functions were measured by the stacked-foil technique for the reactions <sup>76</sup>Se(p, n)<sup>76</sup>Br, <sup>76</sup>Se(p, 2n)<sup>75</sup>Br, <sup>76</sup>Se(p, 3n)<sup>74<em>m</em></sup>Br, <sup>76</sup>Se(p, α)<sup>73</sup>As, <sup>76</sup>Se(p, αn)<sup>72</sup>As, <sup>76</sup>Se(p, α2n)<sup>71</sup>As and <sup>76</sup>Se(p, <sup>3</sup>He + 2pn + pd)<sup>74</sup>As on 96.48% enriched <sup>76</sup>Se up to <em>E</em><sub>p</sub> = 40 MeV. The optimum energy range for the production of <sup>75</sup>Br via the <sup>76</sup>Se(p, 2n)<sup>75</sup>Br reaction at our compact cyclotron is <em>E</em><sub>p</sub> = 24 → 21.5 MeV, the calculated thick target yield of <sup>75</sup>Br amounting to 32 mCi/μ Ah and the expected level of <sup>76</sup>Br-impurity to 2.0%. A thin layer of metallic <sup>76</sup>Se on Al-backing was used as target in combination with a water-cooled rotating target head. A dry distillation technique for the separation of radiobromine from irradiated targets was developed; radiochemical yields of about 40–52% were obtained. Using a 50.2 mg/cm<sup>2</sup> thick target (<em>E</em><sub>p</sub> = 24→21.85 MeV, an irradiation time of 1.25 h at a nominal proton beam current of 15 μA and a distillation time of 30 min at 300°C, about 160 mCi of <sup>75</sup>Br (at EOB) is produced. The total loss of <sup>76</sup>Se after irradiation and distillation process is <1%. The levels of <sup>76</sup>Br and <sup>77</sup>Br impurities in <sup>75</sup>Br are <3% and 0.15%, respectively.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 8","pages":"Pages 635-642"},"PeriodicalIF":0.0,"publicationDate":"1985-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90004-3","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"73150765","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1985-08-01DOI: 10.1016/0020-708X(85)90007-9
Sonja Abram, Ulrich Abram, Hartmut Spies, Rudolf Münze
A series of 7 indiumdialkyldithiocarbamates (R = ethyl, n-propyl, i-propyl, n-butyl, i-butyl, (CH2)5, (CH2)2O(CH2)2) has been prepared by reacting InCl3 with aqueous solutions of the ligands. The products have been investigated at various concentration levels. The properties of the products at the lower concentration levels have been studied by thin-layer chromatography, electrophoresis and by determination of the octanol/water partition. A comparison of the results with the behaviour of the well-characterized tris(dialkyldithiocarbamato)indium(III) complexes is given.
{"title":"113mIn chelate complexes—I. In vitro investigations on a series of alkylvaried dithiocarbamato complexes with 113mIn","authors":"Sonja Abram, Ulrich Abram, Hartmut Spies, Rudolf Münze","doi":"10.1016/0020-708X(85)90007-9","DOIUrl":"10.1016/0020-708X(85)90007-9","url":null,"abstract":"<div><p>A series of 7 indiumdialkyldithiocarbamates (R = ethyl, n-propyl, i-propyl, n-butyl, i-butyl, (CH<sub>2</sub>)<sub>5</sub>, (CH<sub>2</sub>)<sub>2</sub>O(CH<sub>2</sub>)<sub>2</sub>) has been prepared by reacting InCl<sub>3</sub> with aqueous solutions of the ligands. The products have been investigated at various concentration levels. The properties of the products at the lower concentration levels have been studied by thin-layer chromatography, electrophoresis and by determination of the octanol/water partition. A comparison of the results with the behaviour of the well-characterized tris(dialkyldithiocarbamato)indium(III) complexes is given.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 8","pages":"Pages 653-656"},"PeriodicalIF":0.0,"publicationDate":"1985-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90007-9","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84215949","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}