William M Steinberger, Lorenzo Mercolli, Johannes Breuer, Hasan Sari, Szymon Parzych, Szymon Niedzwiecki, Gabriela Lapkiewicz, Pawel Moskal, Ewa Stepien, Axel Rominger, Kuangyu Shi, Maurizio Conti
{"title":"使用长轴视场正电子发射断层扫描仪进行的正电子寿命验证测量。","authors":"William M Steinberger, Lorenzo Mercolli, Johannes Breuer, Hasan Sari, Szymon Parzych, Szymon Niedzwiecki, Gabriela Lapkiewicz, Pawel Moskal, Ewa Stepien, Axel Rominger, Kuangyu Shi, Maurizio Conti","doi":"10.1186/s40658-024-00678-4","DOIUrl":null,"url":null,"abstract":"<p><strong>Background: </strong>Positron emission tomography (PET) traditionally uses coincident annihilation photons emitted from a positron interacting with an electron to localize cancer within the body. The formation of positronium (Ps), a bonded electron-positron pair, has not been utilized in clinical applications of PET due to the need to detect either the emission of a prompt gamma ray or the decay of higher-order coincident events. Assessment of the lifetime of the formed Ps, however, can potentially yield additional diagnostic information of the surrounding tissue because Ps properties vary due to void size and molecular composition. To assess the feasibility of measuring Ps lifetimes with a PET scanner, experiments were performed in a Biograph Vision Quadra (Siemens Healthineers). Quadra is a long-axial field-of-view (LA-FOV) PET scanner capable of producing list-mode data from single interaction events.</p><p><strong>Results: </strong>Ortho-Ps (o-Ps) lifetimes were measured for quartz-glass and polycarbonate samples using a <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>22</mn></mmultiscripts> <mtext>Na</mtext></mrow> </math> positron source. Results produced o-Ps lifetimes of 1.538 ± 0.036 ns for the quartz glass and 1.927 ± 0.042 ns for the polycarbonate. Both o-Ps lifetimes were determined using a double-exponential fit to the time-difference distribution between the emission of a prompt gamma ray and the annihilation of the correlated positron. The measured values match within a single standard deviation of previously published results. The quartz-glass samples were additional measured with <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>82</mn></mmultiscripts> <mtext>Rb</mtext></mrow> </math> , <math><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>68</mn></mmultiscripts> </math> Ga and <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>124</mn></mmultiscripts> <mtext>I</mtext></mrow> </math> to validate the lifetime using clinically available sources. A double-exponential fit was initially chosen as a similar methodology to previously published works, however, an exponentially-modified Gaussian distribution fit to each lifetime more-accurately models the data. A Bayesian method was used to estimate the variables of the fit and o-Ps lifetime results are reported using this methodology for the three clinical isotopes: 1.59 ± 0.03 ns for <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>82</mn></mmultiscripts> <mtext>Rb</mtext></mrow> </math> , 1.58 ± 0.07 ns for <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>68</mn></mmultiscripts> <mtext>Ga</mtext></mrow> </math> and 1.62 ± 0.01 ns for <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>124</mn></mmultiscripts> <mtext>I</mtext></mrow> </math> . The impact of scatter and attenuation on the o-Ps lifetime was also assessed by analyzing a water-filled uniform cylinder (20 <math><mi>ϕ</mi></math> <math><mo>×</mo></math> 30 cm <math><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>3</mn></mmultiscripts> </math> ) with an added <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>82</mn></mmultiscripts> <mtext>Rb</mtext></mrow> </math> solution. Lifetimes were extracted for various regions of the cylinder and while there is a shape difference in the lifetime due to scatter, the extracted o-Ps lifetime of the water, 1.815 ± 0.013 ns, agrees with previously published results.</p><p><strong>Conclusion: </strong>Overall, the methodology presented in this manuscript demonstrates the repeatability of Ps lifetime measurements with clinically available isotopes in a commercially-available LA-FOV PET scanner. This validation work lays the foundation for future in-vivo patient scans with Quadra.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"76"},"PeriodicalIF":3.0000,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11362402/pdf/","citationCount":"0","resultStr":"{\"title\":\"Positronium lifetime validation measurements using a long-axial field-of-view positron emission tomography scanner.\",\"authors\":\"William M Steinberger, Lorenzo Mercolli, Johannes Breuer, Hasan Sari, Szymon Parzych, Szymon Niedzwiecki, Gabriela Lapkiewicz, Pawel Moskal, Ewa Stepien, Axel Rominger, Kuangyu Shi, Maurizio Conti\",\"doi\":\"10.1186/s40658-024-00678-4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><strong>Background: </strong>Positron emission tomography (PET) traditionally uses coincident annihilation photons emitted from a positron interacting with an electron to localize cancer within the body. The formation of positronium (Ps), a bonded electron-positron pair, has not been utilized in clinical applications of PET due to the need to detect either the emission of a prompt gamma ray or the decay of higher-order coincident events. Assessment of the lifetime of the formed Ps, however, can potentially yield additional diagnostic information of the surrounding tissue because Ps properties vary due to void size and molecular composition. To assess the feasibility of measuring Ps lifetimes with a PET scanner, experiments were performed in a Biograph Vision Quadra (Siemens Healthineers). Quadra is a long-axial field-of-view (LA-FOV) PET scanner capable of producing list-mode data from single interaction events.</p><p><strong>Results: </strong>Ortho-Ps (o-Ps) lifetimes were measured for quartz-glass and polycarbonate samples using a <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>22</mn></mmultiscripts> <mtext>Na</mtext></mrow> </math> positron source. Results produced o-Ps lifetimes of 1.538 ± 0.036 ns for the quartz glass and 1.927 ± 0.042 ns for the polycarbonate. Both o-Ps lifetimes were determined using a double-exponential fit to the time-difference distribution between the emission of a prompt gamma ray and the annihilation of the correlated positron. The measured values match within a single standard deviation of previously published results. The quartz-glass samples were additional measured with <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>82</mn></mmultiscripts> <mtext>Rb</mtext></mrow> </math> , <math><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>68</mn></mmultiscripts> </math> Ga and <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>124</mn></mmultiscripts> <mtext>I</mtext></mrow> </math> to validate the lifetime using clinically available sources. A double-exponential fit was initially chosen as a similar methodology to previously published works, however, an exponentially-modified Gaussian distribution fit to each lifetime more-accurately models the data. A Bayesian method was used to estimate the variables of the fit and o-Ps lifetime results are reported using this methodology for the three clinical isotopes: 1.59 ± 0.03 ns for <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>82</mn></mmultiscripts> <mtext>Rb</mtext></mrow> </math> , 1.58 ± 0.07 ns for <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>68</mn></mmultiscripts> <mtext>Ga</mtext></mrow> </math> and 1.62 ± 0.01 ns for <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>124</mn></mmultiscripts> <mtext>I</mtext></mrow> </math> . The impact of scatter and attenuation on the o-Ps lifetime was also assessed by analyzing a water-filled uniform cylinder (20 <math><mi>ϕ</mi></math> <math><mo>×</mo></math> 30 cm <math><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>3</mn></mmultiscripts> </math> ) with an added <math> <mrow><mmultiscripts><mrow></mrow> <mrow></mrow> <mn>82</mn></mmultiscripts> <mtext>Rb</mtext></mrow> </math> solution. Lifetimes were extracted for various regions of the cylinder and while there is a shape difference in the lifetime due to scatter, the extracted o-Ps lifetime of the water, 1.815 ± 0.013 ns, agrees with previously published results.</p><p><strong>Conclusion: </strong>Overall, the methodology presented in this manuscript demonstrates the repeatability of Ps lifetime measurements with clinically available isotopes in a commercially-available LA-FOV PET scanner. 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引用次数: 0
摘要
背景:正电子发射断层扫描(PET)传统上利用正电子与电子相互作用所发射的重合湮灭光子来定位体内的癌症。正电子(Ps)是一种键合的电子-正电子对,由于需要检测瞬时伽马射线的发射或高阶重合事件的衰变,因此正电子发射断层扫描的临床应用还没有利用到正电子(Ps)的形成。然而,由于Ps的特性会因空隙大小和分子组成的不同而变化,因此评估形成的Ps的寿命有可能获得有关周围组织的额外诊断信息。为了评估使用 PET 扫描仪测量 Ps 寿命的可行性,我们在 Biograph Vision Quadra(西门子医疗集团)中进行了实验。Quadra 是一种长轴视场(LA-FOV)PET 扫描仪,能够从单次相互作用事件中生成列表模式数据:结果:使用 22 Na 正电子源测量了石英玻璃和聚碳酸酯样品的正负电子寿命(o-Ps)。结果显示,石英玻璃的 o-Ps 寿命为 1.538 ± 0.036 ns,聚碳酸酯的 o-Ps 寿命为 1.927 ± 0.042 ns。这两个 o-Ps 寿命都是通过双指数拟合瞬时伽马射线发射与相关正电子湮灭之间的时差分布确定的。测量值与之前公布的结果相差一个标准差。石英玻璃样品还用 82 Rb、68 Ga 和 124 I 进行了额外测量,以利用临床可用的放射源验证寿命。最初选择的双指数拟合方法与之前发表的研究结果类似,但对每个寿命进行指数修正的高斯分布拟合能更准确地模拟数据。使用贝叶斯方法估计了拟合变量,并报告了使用该方法对三种临床同位素的 o-Ps 寿命结果:82 Rb 为 1.59 ± 0.03 ns,68 Ga 为 1.58 ± 0.07 ns,124 I 为 1.62 ± 0.01 ns。散射和衰减对 o-Ps 寿命的影响也通过分析加入了 82 Rb 溶液的充水均匀圆柱体(20 ϕ × 30 cm 3)来评估。虽然由于散射的原因,o-Ps 寿命在形状上存在差异,但提取的水的 o-Ps 寿命(1.815 ± 0.013 ns)与之前公布的结果一致:总之,本手稿中介绍的方法证明了在商用 LA-FOV PET 扫描仪中使用临床可用同位素测量 Ps 寿命的可重复性。这项验证工作为将来使用 Quadra 进行体内患者扫描奠定了基础。
Positronium lifetime validation measurements using a long-axial field-of-view positron emission tomography scanner.
Background: Positron emission tomography (PET) traditionally uses coincident annihilation photons emitted from a positron interacting with an electron to localize cancer within the body. The formation of positronium (Ps), a bonded electron-positron pair, has not been utilized in clinical applications of PET due to the need to detect either the emission of a prompt gamma ray or the decay of higher-order coincident events. Assessment of the lifetime of the formed Ps, however, can potentially yield additional diagnostic information of the surrounding tissue because Ps properties vary due to void size and molecular composition. To assess the feasibility of measuring Ps lifetimes with a PET scanner, experiments were performed in a Biograph Vision Quadra (Siemens Healthineers). Quadra is a long-axial field-of-view (LA-FOV) PET scanner capable of producing list-mode data from single interaction events.
Results: Ortho-Ps (o-Ps) lifetimes were measured for quartz-glass and polycarbonate samples using a positron source. Results produced o-Ps lifetimes of 1.538 ± 0.036 ns for the quartz glass and 1.927 ± 0.042 ns for the polycarbonate. Both o-Ps lifetimes were determined using a double-exponential fit to the time-difference distribution between the emission of a prompt gamma ray and the annihilation of the correlated positron. The measured values match within a single standard deviation of previously published results. The quartz-glass samples were additional measured with , Ga and to validate the lifetime using clinically available sources. A double-exponential fit was initially chosen as a similar methodology to previously published works, however, an exponentially-modified Gaussian distribution fit to each lifetime more-accurately models the data. A Bayesian method was used to estimate the variables of the fit and o-Ps lifetime results are reported using this methodology for the three clinical isotopes: 1.59 ± 0.03 ns for , 1.58 ± 0.07 ns for and 1.62 ± 0.01 ns for . The impact of scatter and attenuation on the o-Ps lifetime was also assessed by analyzing a water-filled uniform cylinder (20 30 cm ) with an added solution. Lifetimes were extracted for various regions of the cylinder and while there is a shape difference in the lifetime due to scatter, the extracted o-Ps lifetime of the water, 1.815 ± 0.013 ns, agrees with previously published results.
Conclusion: Overall, the methodology presented in this manuscript demonstrates the repeatability of Ps lifetime measurements with clinically available isotopes in a commercially-available LA-FOV PET scanner. This validation work lays the foundation for future in-vivo patient scans with Quadra.
期刊介绍:
EJNMMI Physics is an international platform for scientists, users and adopters of nuclear medicine with a particular interest in physics matters. As a companion journal to the European Journal of Nuclear Medicine and Molecular Imaging, this journal has a multi-disciplinary approach and welcomes original materials and studies with a focus on applied physics and mathematics as well as imaging systems engineering and prototyping in nuclear medicine. This includes physics-driven approaches or algorithms supported by physics that foster early clinical adoption of nuclear medicine imaging and therapy.