Semi Helin, Johan Rajander, Jussi Aromaa, Eveliina Arponen, Jatta S. Helin, Olof Solin
{"title":"氮氢气靶靶内产生的[11C]CH4与束流、辐照时间和靶温的函数关系","authors":"Semi Helin, Johan Rajander, Jussi Aromaa, Eveliina Arponen, Jatta S. Helin, Olof Solin","doi":"10.1186/s41181-024-00255-1","DOIUrl":null,"url":null,"abstract":"<div><h3>Background</h3><p>Production of [<sup>11</sup>C]CH<sub>4</sub> from gas targets is notorious for weak performance with respect to yield, especially when using high beam currents. Post-target conversion of [<sup>11</sup>C]CO<sub>2</sub> to [<sup>11</sup>C]CH<sub>4</sub> is a widely used roundabout method in <sup>11</sup>C-radiochemistry, but the added complexity increase the challenge to control carrier carbon. Thus in-target-produced [<sup>11</sup>C]CH<sub>4</sub> is superior with respect to molar activity. We studied the in-target production of [<sup>11</sup>C]CO<sub>2</sub> and [<sup>11</sup>C]CH<sub>4</sub> from nitrogen gas targets as a function of beam current, irradiation time, and target temperature.</p><h3>Results</h3><p>[<sup>11</sup>C]CO<sub>2</sub> production was practically unchanged across the range of varied parameters, but the [<sup>11</sup>C]CH<sub>4</sub> yield, presented in terms of saturation yield Y<sub>SAT</sub>(<sup>11</sup>CH<sub>4</sub>), had a negative correlation with beam current and a positive correlation with target chamber temperature. A formulated model equation indicates behavior where the [<sup>11</sup>C]CH<sub>4</sub> formation follows a parabolic graph as a function of beam current. The negative square term, i.e., the yield loss, is postulated to arise from Haber–Bosch-like NH<sub>3</sub> formation: N<sub>2</sub> + 3H<sub>2</sub> → 2NH<sub>3</sub>. The studied conditions suggest that the NH<sub>3</sub> (liq.) would be condensed on the target chamber walls, thus depleting the hydrogen reserve needed for the conversion of nascent <sup>11</sup>C to [<sup>11</sup>C]CH<sub>4</sub>.</p><h3>Conclusions</h3><p>[<sup>11</sup>C]CH<sub>4</sub> production can be improved by increasing the target chamber temperature, which is presented in a mathematical formula. Our observations have implications for targetry design (geometry, gas volume and composition, pressure) and irradiation conditions, providing specific knowledge to enhance [<sup>11</sup>C]CH<sub>4</sub> production at high beam currents. Increased [<sup>11</sup>C]CH<sub>4</sub> radioactivity is an obvious benefit in radiosynthesis in terms of product yield and molar radioactivity.</p></div>","PeriodicalId":534,"journal":{"name":"EJNMMI Radiopharmacy and Chemistry","volume":"9 1","pages":""},"PeriodicalIF":4.4000,"publicationDate":"2024-03-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ejnmmipharmchem.springeropen.com/counter/pdf/10.1186/s41181-024-00255-1","citationCount":"0","resultStr":"{\"title\":\"In-target production of [11C]CH4 from a nitrogen/hydrogen gas target as a function of beam current, irradiation time, and target temperature\",\"authors\":\"Semi Helin, Johan Rajander, Jussi Aromaa, Eveliina Arponen, Jatta S. Helin, Olof Solin\",\"doi\":\"10.1186/s41181-024-00255-1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><h3>Background</h3><p>Production of [<sup>11</sup>C]CH<sub>4</sub> from gas targets is notorious for weak performance with respect to yield, especially when using high beam currents. Post-target conversion of [<sup>11</sup>C]CO<sub>2</sub> to [<sup>11</sup>C]CH<sub>4</sub> is a widely used roundabout method in <sup>11</sup>C-radiochemistry, but the added complexity increase the challenge to control carrier carbon. Thus in-target-produced [<sup>11</sup>C]CH<sub>4</sub> is superior with respect to molar activity. We studied the in-target production of [<sup>11</sup>C]CO<sub>2</sub> and [<sup>11</sup>C]CH<sub>4</sub> from nitrogen gas targets as a function of beam current, irradiation time, and target temperature.</p><h3>Results</h3><p>[<sup>11</sup>C]CO<sub>2</sub> production was practically unchanged across the range of varied parameters, but the [<sup>11</sup>C]CH<sub>4</sub> yield, presented in terms of saturation yield Y<sub>SAT</sub>(<sup>11</sup>CH<sub>4</sub>), had a negative correlation with beam current and a positive correlation with target chamber temperature. A formulated model equation indicates behavior where the [<sup>11</sup>C]CH<sub>4</sub> formation follows a parabolic graph as a function of beam current. The negative square term, i.e., the yield loss, is postulated to arise from Haber–Bosch-like NH<sub>3</sub> formation: N<sub>2</sub> + 3H<sub>2</sub> → 2NH<sub>3</sub>. The studied conditions suggest that the NH<sub>3</sub> (liq.) would be condensed on the target chamber walls, thus depleting the hydrogen reserve needed for the conversion of nascent <sup>11</sup>C to [<sup>11</sup>C]CH<sub>4</sub>.</p><h3>Conclusions</h3><p>[<sup>11</sup>C]CH<sub>4</sub> production can be improved by increasing the target chamber temperature, which is presented in a mathematical formula. Our observations have implications for targetry design (geometry, gas volume and composition, pressure) and irradiation conditions, providing specific knowledge to enhance [<sup>11</sup>C]CH<sub>4</sub> production at high beam currents. Increased [<sup>11</sup>C]CH<sub>4</sub> radioactivity is an obvious benefit in radiosynthesis in terms of product yield and molar radioactivity.</p></div>\",\"PeriodicalId\":534,\"journal\":{\"name\":\"EJNMMI Radiopharmacy and Chemistry\",\"volume\":\"9 1\",\"pages\":\"\"},\"PeriodicalIF\":4.4000,\"publicationDate\":\"2024-03-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://ejnmmipharmchem.springeropen.com/counter/pdf/10.1186/s41181-024-00255-1\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"EJNMMI Radiopharmacy and Chemistry\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://link.springer.com/article/10.1186/s41181-024-00255-1\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"CHEMISTRY, INORGANIC & NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"EJNMMI Radiopharmacy and Chemistry","FirstCategoryId":"1085","ListUrlMain":"https://link.springer.com/article/10.1186/s41181-024-00255-1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
In-target production of [11C]CH4 from a nitrogen/hydrogen gas target as a function of beam current, irradiation time, and target temperature
Background
Production of [11C]CH4 from gas targets is notorious for weak performance with respect to yield, especially when using high beam currents. Post-target conversion of [11C]CO2 to [11C]CH4 is a widely used roundabout method in 11C-radiochemistry, but the added complexity increase the challenge to control carrier carbon. Thus in-target-produced [11C]CH4 is superior with respect to molar activity. We studied the in-target production of [11C]CO2 and [11C]CH4 from nitrogen gas targets as a function of beam current, irradiation time, and target temperature.
Results
[11C]CO2 production was practically unchanged across the range of varied parameters, but the [11C]CH4 yield, presented in terms of saturation yield YSAT(11CH4), had a negative correlation with beam current and a positive correlation with target chamber temperature. A formulated model equation indicates behavior where the [11C]CH4 formation follows a parabolic graph as a function of beam current. The negative square term, i.e., the yield loss, is postulated to arise from Haber–Bosch-like NH3 formation: N2 + 3H2 → 2NH3. The studied conditions suggest that the NH3 (liq.) would be condensed on the target chamber walls, thus depleting the hydrogen reserve needed for the conversion of nascent 11C to [11C]CH4.
Conclusions
[11C]CH4 production can be improved by increasing the target chamber temperature, which is presented in a mathematical formula. Our observations have implications for targetry design (geometry, gas volume and composition, pressure) and irradiation conditions, providing specific knowledge to enhance [11C]CH4 production at high beam currents. Increased [11C]CH4 radioactivity is an obvious benefit in radiosynthesis in terms of product yield and molar radioactivity.