Short-lived positron emitters in beam-on PET imaging during proton therapy
- 5 November 2015
- journal article
- Published by IOP Publishing in Physics in Medicine & Biology
- Vol. 60 (23) , 8923-8947
Abstract
The only method for in vivo dose delivery verification in proton beam radiotherapy in clinical use today is positron emission tomography (PET) of the positron emitters produced in the patient during irradiation. PET imaging while the beam is on (so called beam-on PET) is an attractive option, providing the largest number of counts, the least biological washout and the fastest feedback. In this implementation, all nuclides, independent of their half-life, will contribute. As a first step towards assessing the relevance of short-lived nuclides (half-life shorter than that of 10 C, T 1/2 = 19 s) for in vivo dose delivery verification using beam-on PET, we measured their production in the stopping of 55 MeV protons in water, carbon, phosphorus and calcium The most copiously produced short-lived nuclides and their production rates relative to the relevant long-lived nuclides are: 12 N ( T 1/2 = 11 ms) on carbon (9% of 11 C), 29 P ( T 1/2 = 4.1 s) on phosphorus (20% of 30 P) and 38m K ( T 1/2 = 0.92 s) on calcium (113% of 38g K). No short-lived nuclides are produced on oxygen. The number of decays integrated from the start of an irradiation as a function of time during the irradiation of PMMA and 4 tissue materials has been determined. For (carbon-rich) adipose tissue, 12 N dominates up to 70 s. On bone tissue, 12 N dominates over 15 O during the first 8–15 s (depending on carbon-to-oxygen ratio). The short-lived nuclides created on phosphorus and calcium provide 2.5 times more beam-on PET counts than the long-lived ones produced on these elements during a 70 s irradiation. From the estimated number of 12 N PET counts, we conclude that, for any tissue, 12 N PET imaging potentially provides equal to superior proton range information compared to prompt gamma imaging with an optimized knife-edge slit camera. The practical implementation of 12 N PET imaging is discussed.Keywords
This publication has 43 references indexed in Scilit:
- Ionoacoustic characterization of the proton Bragg peak with submillimeter accuracyMedical Physics, 2015
- Time-of-flight neutron rejection to improve prompt gamma imaging for proton range verification: a simulation studyPhysics in Medicine & Biology, 2012
- Direct time-of-flight for quantitative, real-time in-beam PET: a concept and feasibility studyPhysics in Medicine & Biology, 2007
- On the detector arrangement for in-beam PET for hadron therapy monitoringPhysics in Medicine & Biology, 2006
- Suppression of random coincidences during in-beam PET measurements at ion beam radiotherapy facilitiesIEEE Transactions on Nuclear Science, 2005
- Geant4—a simulation toolkitNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2003
- Absolute full-energy peak efficiency calibration of a Clover–BGO detector systemNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2003
- The Clover: a new generation of composite Ge detectorsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1999
- Energy levels of light nuclei A = 5−10Nuclear Physics A, 1988
- Mathematical Removal of Positron Range Blurring in High Resolution TomographyIEEE Transactions on Nuclear Science, 1986