The well-established use of 125I and 111In, Auger-emitting radioisotopes, has also stimulated the search for other Auger emitters that may be more practical to use from the perspective of availability, physical half-life, and cost. In our work, we proposed a 109Pd/109mAg in-vivo generator that combines β− emission from the parent 109Pd radionuclide with a high emission of Auger electrons from the daughter 109mAg. In our concept, the 109Pd/109mAg in-vivo generator was applied in the form of Au@109Pd core-shell nanoparticles. We found that complete retention of 109mAg was accomplished following the nuclear decay of the immobilized 109Pd on the AuNPs surface. This contrasts with previously published data for chelator-based in-vivo generators. Studies conducted on in vivo generators, such as 103Pd/103mRh (Jensen et al. 2020), 166Dy/166Ho (Wang et al. 2022) and 212Pb/212Bi (Mirzadeh et al. 1993), have demonstrated that a significant percentage of daughter radionuclides are liberated when chelators are employed to immobilize parent radionuclides. According to (Wang et al. 2022), the loss of daughter radionuclides was attributed to their de-excitation through the internal conversion, resulting in Auger electron emission, rather than to the recoil energy associated with the emission of ß- particles and neutrinos. As a result, the de-excited daughter radionuclides become highly charged what leads to electrons uptake from the surrounding chelator donor atoms. Moreover, due to the electron transfer to highly charged atoms, donor atoms of chelators acquire a positive charge. The metal-ligand bonds are then broken as a result of the repulsive force between the positively charged atoms, and the daughter radionuclides are released as free cations.
The situation changes dramatically when the parent radionuclide is immobilized on a metallic surface instead of a chelate complex. The application of a metallic surface such as AuNPs as the carrier of the mother radionuclides facilitates the availability of several delocalized electrons. After nuclear decay, highly positively charged daughter radionuclide takes electrons from neighboring Au atoms on the surface. As a result, the positive charge is rapidly transferred to the entire nanoparticle, causing only a marginal change in the surface charge. Therefore, the release of 109mAg from the nanoparticles surface is not achievable. The same effect was also observed] with the 166Dy/166Ho in vivo generator deposited on the AuNPs surface (Wang et al. 2022).
This phenomenon is advantageous from the perspective of potential applications. As 109mAg remains in the NPs structure, there is negligible risk of 109Ag unspecific accumulation in different tissues after treatment. Thus, it significantly limits the risks of post treatment side-effects related to increased and difficult to detect silver accumulation throughout the patient organism.
In performed in vitro studies, we observe the crucial role of the trastuzumab vector, which facilitates the cell internalization and cytoplasm localization of Au@109Pd-trastuzumab conjugate into the SKOV-3 cells. As presented in confocal images (Fig. 5), the conjugate accumulates in the perinuclear area surrounding the cell nucleus. In the case of β− radiation, due to the fact that the range of β− radiation emitted by 109Pd is a few millimeters, cell internalization is not necessary, and the β− particles are capable of targeting DNA without cell internalization of 109Pd. This explains why we observed also cytotoxicity for Au@109Pd-PEG nanoparticles. Considering the low-LET characteristics of β− radiation, a significantly lower DNA DSB generation yield is expected, leading to a lower overall toxicity ratio. However, the interaction of Auger electrons with the essential cell components is required to induce the cytotoxic effect correlated with the Auger electron emission from 109mAg as the daughter radionuclide. Cellular DNA is typically considered to be the most sensitive target of Auger electron emitters. The double-stranded DNA helix possesses a diameter of 2 nm. During a typical Auger emission, the greatest release of energy happens in 1–2 nm spheres around the decay site (Buchegger et al. 2006). Similar to the α-radiation path through the cell nucleus, the loss of genetic information occurs in these double-strand breaks, which is attributed to the nucleotide breakdown on both strands (Lobachevsky, et al. 2000). For 125I decays associated with DNA, it means "One decay = one double-strand break" (Elmroth et al 2005). Furthermore, as has been proposed in some publications, since the cell membrane plays a key role in cell viability, the effects of Auger electrons generated by membrane-bound radiolabeled mAbs should not be overlooked (Pouget et al. 2008; Paillas et al 2016, Muller et al. 2022). Considering the significant accumulation of nanoparticles on the nuclear membrane within the range of Auger and conversion electron interaction as depicted in confocal microscopy images (Fig. 5), it has been concluded that nuclear envelope damage caused by Auger electrons may be one of numerous reasons of cell death. In order to verify the therapy enhancement for simultaneous β− particle emission and conversion/Auger electrons, we decided to perform a comparable analysis with 125I (Auger) and 198Au (β−) radionuclides. Both of them were directly implemented into the nanoparticle structure by chemisorption of iodine (125I-labeled Au@Pd-trastuzumab (supp.info)) or by using radioactive 198AuNPs-trastuzumab radiobioconjugates, as we previously described [Żelechowska-Matysiak et al. 2023).
Table 2
Comparison of cytotoxicity of radiobioconjugates labeled with Auger electron emitter (125I), β-emitter (198Au) and Auger and β-electron emitter (109Pd/109mAg in vivo generator). Activity concentration: 20 MBq/ml, incubation time: 48 h.
Radiobioconjugate | T1/2 (days) | Decay mode | Decay numer in 48 h | Radiation emitted | % of metabolic activity in MTS test |
Au@Pd125I-trastuzumab | 59.49 | EC | 3.42x1012 | Auger, low energy gamma | 60 |
198Au-trastuzumab | 2.69 | β− | 2.70x1012 | β−avg (315 keV) | 53 |
Au@109Pd-trastuzumab | 0.57 | β−, IT | 1.30x1012 | β−avg (436 keV) + Auger/conversion | 10 |
The comparison provided in Table 2 is undoubtedly an approximation. It does not take into account several parameters, including radionuclide half-life, radiation intensity and energy. In addition, the emitted γ radiation was not taken into account, considering its insignificance in relation to the corpuscular radiation.We intended to compare the obtained data with currently existing alternative pathways. The acquired results, however, clearly reveal that the cytotoxicity of the 109Pd/109mAg in vivo generator-based conjugate (β- and Auger electron emitter) is significantly higher than that of the conjugates radiolabeled with the same activities of β− or Auger electron emitters. This effect will be much greater if the considerably shorter half-life of 109Pd is taken into account.