<p>This study demonstrates the applicability of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(^{52}\)</EquationSource> </InlineEquation>Mn and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(^{55}\)</EquationSource> </InlineEquation>Co radionuclides for positronium imaging. Positronium Lifetime Imaging (PLI) extends positron emission tomography by using the lifetime of positronium atoms as a probe of tissue molecular architecture. However, its practical use requires <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\beta ^{+}\)</EquationSource> </InlineEquation> emitters that also provide an additional prompt <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> </InlineEquation> ray to mark the positron creation time. In this work, we report the first PLI measurements performed with <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(^{52}\)</EquationSource> </InlineEquation>Mn and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(^{55}\)</EquationSource> </InlineEquation>Co using the modular J-PET. Four samples were studied in each experiment: two Certified Reference Materials (polycarbonate and fused silica) and two human tissues (cardiac myxoma and adipose). The selection of PLI events was based on the registration of two 511&#xa0;keV annihilation photons and one prompt gamma in triple coincidence. From the resulting lifetime spectra we extracted the mean ortho-positronium lifetime <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\tau _{\text {oPs}}\)</EquationSource> </InlineEquation> and the mean positron lifetime <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\Delta T_{\text {mean}}\)</EquationSource> </InlineEquation> for each sample. The measured values of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\tau _{\text {oPs}}\)</EquationSource> </InlineEquation> in polycarbonate using both isotopes matches well with the certified reference values. Furthermore, <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(^{55}\)</EquationSource> </InlineEquation>Co reproduced identical results for fused-silica measurements at their respective uncertainty levels. In contrast, measurements with <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(^{52}\)</EquationSource> </InlineEquation>Mn in fused silica show a minor deviation, which could be caused by the Parafilm spacer. In myxoma and adipose tissue, the reduced <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\tau _{\text {oPs}}\)</EquationSource> </InlineEquation> values are mainly linked to the long storage history of the samples rather than to the choice of isotope. Comparing peak-to-background ratios and spectral purity, <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{55}\)</EquationSource> </InlineEquation>Co provides cleaner PLI data under the same experimental conditions. Although <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(^{52}\)</EquationSource> </InlineEquation>Mn offers a longer half-life and a multi gamma cascade enhancing <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\beta ^{+}\)</EquationSource> </InlineEquation> + <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> </InlineEquation> coincidences, but at the expense of higher background. In this study, we demonstrate that the applied selection criteria on the data measured with the modular J-PET can be used for PLI studies even with radionuclides with complex decay patterns.</p>

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First positronium lifetime imaging using 52Mn and 55Co with a plastic-scintillator-based PET scanner

  • Manish Das,
  • Sushil Sharma,
  • Ermias Yitayew Beyene,
  • Aleksander Bilewicz,
  • Jarosław Choiński,
  • Neha Chug,
  • Catalina Curceanu,
  • Eryk Czerwiński,
  • Jakub Hajduga,
  • Sharareh Jalali,
  • Krzysztof Kacprzak,
  • Tevfik Kaplanoglu,
  • Łukasz Kapłon,
  • Kamila Kasperska,
  • Aleksander Khreptak,
  • Grzegorz Korcyl,
  • Tomasz Kozik,
  • Karol Kubat,
  • Deepak Kumar,
  • Sumit Kumar Kundu,
  • Anoop Kunimmal Venadan,
  • Edward Lisowski,
  • Filip Lisowski,
  • Justyna Medrala-Sowa,
  • Simbarashe Moyo,
  • Wiktor Mryka,
  • Szymon Niedźwiecki,
  • Anand Pandey,
  • Piyush Pandey,
  • Szymon Parzych,
  • Alessio Porcelli,
  • Bartłomiej Rachwał,
  • Martin Rädler,
  • Narendra Rathod,
  • Noman Razzaq,
  • Axel Rominger,
  • Kuangyu Shi,
  • Magdalena Skurzok,
  • Maciej Słotwiński,
  • Anna Stolarz,
  • Tomasz Szumlak,
  • Pooja Tanty,
  • Keyvan Tayefi Ardebili,
  • Satyam Tiwari,
  • Kavya Valsan Eliyan,
  • Rafał Walczak,
  • Ewa Ł. Stepień,
  • Paweł Moskal

摘要

This study demonstrates the applicability of \(^{52}\) Mn and \(^{55}\) Co radionuclides for positronium imaging. Positronium Lifetime Imaging (PLI) extends positron emission tomography by using the lifetime of positronium atoms as a probe of tissue molecular architecture. However, its practical use requires \(\beta ^{+}\) emitters that also provide an additional prompt \(\gamma\) ray to mark the positron creation time. In this work, we report the first PLI measurements performed with \(^{52}\) Mn and \(^{55}\) Co using the modular J-PET. Four samples were studied in each experiment: two Certified Reference Materials (polycarbonate and fused silica) and two human tissues (cardiac myxoma and adipose). The selection of PLI events was based on the registration of two 511 keV annihilation photons and one prompt gamma in triple coincidence. From the resulting lifetime spectra we extracted the mean ortho-positronium lifetime \(\tau _{\text {oPs}}\) and the mean positron lifetime \(\Delta T_{\text {mean}}\) for each sample. The measured values of \(\tau _{\text {oPs}}\) in polycarbonate using both isotopes matches well with the certified reference values. Furthermore, \(^{55}\) Co reproduced identical results for fused-silica measurements at their respective uncertainty levels. In contrast, measurements with \(^{52}\) Mn in fused silica show a minor deviation, which could be caused by the Parafilm spacer. In myxoma and adipose tissue, the reduced \(\tau _{\text {oPs}}\) values are mainly linked to the long storage history of the samples rather than to the choice of isotope. Comparing peak-to-background ratios and spectral purity, \(^{55}\) Co provides cleaner PLI data under the same experimental conditions. Although \(^{52}\) Mn offers a longer half-life and a multi gamma cascade enhancing \(\beta ^{+}\) + \(\gamma\) coincidences, but at the expense of higher background. In this study, we demonstrate that the applied selection criteria on the data measured with the modular J-PET can be used for PLI studies even with radionuclides with complex decay patterns.