Production of a broad palette of positron emitting radioisotopes using a low-energy cyclotron: Towards a new success story in cancer imaging?
Introduction
Cancer has become a global menace over the years and in today's world it is a major impediment to social and economic advances. Approximately 38 million people worldwide die of non-communicable diseases (NCDs) every year, out of which more than 9 million deaths are only due to cancer (Cancer Statistics, 2021; Lopez-Gomez et al., 2013; Global Cancer Observatory, 2020; Sung et al., 2021). According to the Global Cancer Observatory, it is estimated that there will be 15–17 million new cancer cases every year, of which 60% will be from the developing countries (Global Cancer Observatory, 2020; Sung et al., 2021). However, cancer related mortality can be significantly reduced provided it is detected at a very early stage. With current resources, one-third of newly diagnosed cancer patients could experience significantly increased survival, thanks to early-stage detection. In this endeavor, molecular imaging technology has emerged as one of the main pillars of comprehensive cancer care facilitating early diagnosis by non-invasive visualization and real time monitoring without tissue destruction (Bhanji et al., 2021; Chen et al., 2014; Jokar et al., 2021; Pysz et al., 2010; Wu and Shu, 2018).
Among the various molecular imaging modalities, positron emission tomography (PET) offers picomolar sensitivity and is a fully translational technique (Bhanji et al., 2021; Dagallier et al., 2021; Li and Conti, 2010; Slart et al., 2021; Zanoni et al., 2021). This approach requires specific molecular probes radiolabeled with positron-emitting radioisotopes having suitable radioactive decay parameters. The radioisotope incorporated in the molecular probe decays resulting in the emission of positrons which interact with nearby electrons after travelling a short distance (~ 1 mm) within the body. Each positron-electron annihilation process produces two γ-photons each of 511-keV in opposite directions, which are detected by the detectors surrounding the subject to precisely locate the source of the decay event (Fig. 1A). Subsequently, the ‘coincidence events’ data can be processed by computers to reconstruct the spatial distribution of the radiolabeled molecular probes and the PET images thus generated can reflect the concentration and in vivo distribution of the radiotracer administered (Fig. 1B). This technology provides highly sensitive and quantitative information and is playing an increasingly important role in earlier disease detection and improved therapeutic decision making.
Over the last three decades, PET has matured from a largely obscure and experimental technology to an indispensable constituent of routine nuclear medicine practices. Driving this transition, in part, have been mutually necessary advances in instrumentation and biomedical engineering, radiopharmaceutical chemistry and cancer biology. Somewhat unsung has been the seminal role of radioisotope production technology in fostering the availability of new PET radiotracers for improved cancer imaging and this review is an attempt to rectify this oversight. The positron emitting radioisotopes used for PET, being neutron deficient, are generally produced in cyclotron. Presently, more and more countries around the world are investing heavily on installation and commissioning of new cyclotron facilities, which are mostly low energy cyclotrons exclusively for production of medically important radioisotopes. In this review, we will first discuss the criteria for radioisotope selection for PET imaging. Then, we categorize the positron emitting radioisotopes produced in low energy cyclotrons as: established, emerging and futuristic. Thereafter, we discuss briefly regarding the production methodologies and the radiochemical separation procedures for obtaining the radioisotopes in a form suitable for preparation of radiopharmaceuticals for PET imaging.
Section snippets
Radioisotope selection for PET
The choice of the radioisotope for PET imaging is guided by its nuclear decay properties, chemical characteristics, availability and time-scale of the studied biological process (Li and Conti, 2010). Precisely, the choice of radioisotope depends on its physical half-life, which should not only allow sufficient time for the radiolabeling reactions for formulation of radiopharmaceuticals but also match the pharmacokinetics of the corresponding biological tracers in order to obtain decent
Classification of radioisotopes
There are several categories of positron emitting radioisotopes. Few of them, such as 18F and 68Ga have been well established in clinical context and there are approved radiopharmaceuticals available in the commercial market (Coenen et al., 2010; Smith et al., 2013; Surasi et al., 2014). In case of certain radioisotopes such as 64Cu, 89Zr and 124I, there is emerging clinical interest and presently, clinical trials are going on in different parts of the world (Deri et al., 2013; Nagarajah et
Conclusions
In the preceding pages, it was our aim to shed light not only on the critical role that production methodologies of positron emitting radioisotopes has played towards synthesis and development of novel PET imaging agents but also showcase the power and promise of the new radioisotopes for translation to the clinic in future. This mini review clearly illustrates that the diversity in nuclear decay characteristics of the radioisotopes and their viable and cost-effective production routes (using
Authorship contribution statement
Rubel Chakravarty: Conceptualization, Writing - original draft.
Sudipta Chakraborty: Writing - review & editing.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
The authors are thankful to Dr. P. K. Pujari, Director, Radiochemistry and Isotope Group, Bhabha Atomic Research Centre for his valuable guidance and support to the Isotope Program.
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