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Erschienen in: Journal of Nanoparticle Research 6/2012

01.06.2012 | Research Paper

Radiolabelling of nanoparticles by proton irradiation: temperature control in nanoparticulate powder targets

verfasst von: Uwe Holzwarth, Antonio Bulgheroni, Neil Gibson, Jan Kozempel, Giulio Cotogno, Kamel Abbas, Federica Simonelli, Izabela Cydzik

Erschienen in: Journal of Nanoparticle Research | Ausgabe 6/2012

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Abstract

Radiolabelled nanoparticles are useful tools for biodistribution or cellular uptake studies related to the risk assessment of nanomaterials. Such studies are ideally carried out with industrially manufactured nanoparticles. Irradiation of small quantities of such nanoparticles, in the form of dry powders, with neutrons or light ions allows radiolabelling while preserving their biologically relevant properties. However, nanoparticle powders exhibit poor thermal conductivity and may overheat under irradiation. Their effective thermal conductivity is not known and conventional temperature measurement methods are difficult to apply. Reasonably accurate temperature data could be derived from post-irradiation X-ray diffraction studies on anatase ST-01 TiO2-nanoparticles, with a primary particle size of 7 nm, subjected to proton beams of different intensities. The anatase-to-rutile phase transition starting at about 750 °C was identified by observing rutile peaks in X-ray diffraction patterns. The onset of growth of single diffracting TiO2-domains at around 200 °C was revealed by shape analysis of the diffraction peaks. Identifying these reference temperatures allowed a calibration of the calculated temperature profile. The effective thermal conductivity in the TiO2 powder target was found to be close to that of air trapped in interstices of the nanoparticulate powder. This suggests that the contribution of the nanoparticles to the heat removal from the target is negligible, thus necessitating the use of thin nanoparticle layers in the target in order to facilitate cooling and prevent thermally induced alterations of the nanoparticles.

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1
Atoms may also be displaced from their crystal lattice sites following collisions with primary ions and recoiling atoms (Gibson et al. 2011). The effects of this classical radiation damage and the effects of stopping ions in individual NPs depends critically on NP size. This will be treated in a forthcoming article.
 
2
The notation 48Ti(p,n)48V describes the nuclear reaction of a 48Ti atom with a proton (p) in which a radioactive 48V atom is created and a neutron (n) is emitted. Thus, the number of nucleons remains 48 but one neutron has been replaced by a proton and the Ti atom is transformed into a V atom. The probability of a nuclear reaction to occur is described by the nuclear reaction cross section expressed in barn (1 b = 10−24 cm−2) or millibarn (mb). It can be though of as the circular area corresponding to an effective target area of a 48Ti target atom. A nuclear reaction occurs if a projectile collides with a target atom within this area. Thus, the larger this area the more probable is a nuclear reaction leading to 48V.
 
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Metadaten
Titel
Radiolabelling of nanoparticles by proton irradiation: temperature control in nanoparticulate powder targets
verfasst von
Uwe Holzwarth
Antonio Bulgheroni
Neil Gibson
Jan Kozempel
Giulio Cotogno
Kamel Abbas
Federica Simonelli
Izabela Cydzik
Publikationsdatum
01.06.2012
Verlag
Springer Netherlands
Erschienen in
Journal of Nanoparticle Research / Ausgabe 6/2012
Print ISSN: 1388-0764
Elektronische ISSN: 1572-896X
DOI
https://doi.org/10.1007/s11051-012-0880-y

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