13–19 Apr 2025
Hotel Continental, Ischia Island (Naples, Italy)
Europe/Rome timezone

Production of C-11 for PET imaging using a HRR laser-driven proton source

15 Apr 2025, 17:00
1h 40m
Hotel Continental, Ischia Island (Naples, Italy)

Hotel Continental, Ischia Island (Naples, Italy)

Poster (student) Applications Poster Session

Speaker

Alicia Reija (Galician Institute of High Energy Physics (IGFAE))

Description

In recent years, laser-driven ion accelerators have gained significant interest as an alternative to conventional accelerators. A promising application is the production of radionuclides for medical theragnostics, such as ¹¹C for PET imaging. Currently, these radionuclides are produced in cyclotrons, limiting availability to isotopes with longer lifetime. In this context, compact laser-driven accelerators offer an attractive option for in-situ generation of short-lived isotopes. Although the activities required for PET (>MBq) exceed those achievable from a single laser shot (~kBq), high-power, high-repetition-rate lasers enable continuous production if a suitable target system is developed.
Here, a target assembly based on a rotating wheel and automatic alignment has been designed and commissioned, achieving stable MeV proton acceleration at rates of up to 10 Hz using a 45 TW laser system. Moreover, continuous ¹¹C production via the ¹¹B(p,n)¹¹C reaction was recently demonstrated using the 1 Hz, 1 PW VEGA-3 system (CLPU, Spain), reaching activation levels above 4 MBq. The only current bottleneck to achieving pre-clinical (~10 MBq) PET activities is laser-induced optic heating. Scalability to next-generation laser systems is being explored to assess the feasibility of producing clinical-level (~200 MBq) activities.

Primary authors

A. Bilewicz (Institute of Nuclear Chemistry and Technology, Warwow, Poland) A. Bonasera (Cyclotron Institute, Texas A&M University, College Station, Texas, USA) Aaron Alejo (Instituto Galego de Física de Altas Enerxías (IGFAE), Santiago de Compostela, Spain) Adrián Bembibre Fernández (Instituto Galego de Física de Altas Enerxías (IGFAE). Universidade de Santiago de Compostela (USC)) Alicia Reija (Galician Institute of High Energy Physics (IGFAE)) C. Morgat (Université de Bordeaux, Bordeaux, France) D. Batani (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) D. Dubresson (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) D. Raffestin (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) E. Filippov (CLPU, Villamayor, Salamanca, Spain) G. Lorenzo (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, Dolni Brezany, Czech Republic) H. Larreur (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) J. Benlliure (Instituto de Física Corpuscular, CSIC-Universitat de València, Spain) J.A. Pérez Hernández (CLPU, Villamayor, Salamanca, Spain) Juan Peñas (Instituto Galego de Física de Altas Enerxías (IGFAE)) K. Batani (IPPLM Institute of Plasma Physics and Laser Microfusion, Warsaw, Poland) L. Volpe (CLPU, Villamayor, Salamanca, Spain) M. Dias Rodrigues (Cyclotron Institute, Texas A&M University, College Station, Texas, USA) M. Huault (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) P. Nicolai (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) R. Margnes (CELIA – Université de Bordeaux, CNRS, CEA, UMR 5107, Talence, France) V. Kantarelou (ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, Dolni Brezany, Czech Republic)

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