Experimental study on microSPECT-CT bremsstrahlung imaging in solid tumor mesenchymal implantation of 32 P-chromic phosphate-paclitaxel-poly-L-lactic acid sustained-release seeds / 重庆医学

Objective To investigate the value of single photon emission computed tomography (CT) imaging and transmis‐sion CT imaging (microSPECT‐CT ) bremsstrahlung imaging for the solid tumor mesenchymal implantaion of 32 P‐chromic phos‐phate‐paclitaxel‐poly‐L‐lactic acid (32 P‐CP‐PSP‐PLLA) sustained release seeds and to investigate the 32 P in vivo biodistribution and degradation sustained release churacteristics .Methods The animal model of prostate cancer subcutaneously transplanted tumor was established .32 P‐CP‐PSP‐PLLA sustained‐release seeds were intratumorally implanted by the mediation of microSPECT‐CT brems‐strahlung imaging and the 32 P distribution in bearing tumor mouse was verified by the imaging and biological distrubtion tests .The ultrastructural changes of 32 P seeds were observed by the scanning electron microscope .Results The MicroSPECT/CT brems‐strahlung imaging could effectively guide the intratumoral implantation operation of the 32 P sustained‐release seeds with clear visu‐alization .Partial sustained‐release 32 P was remained in the tumor tissues with little distribution in important organs of spleen and liver ,which was proved by the biodistribution results .The particle surface and inside micropores and tunnels formation ,their pro‐gressive increase ,fusion and connection were found by the electronic microscope after the 32 P sustained‐release seeds intratumoral implantation .Conclusion The MicroSPECT/CT bremsstrahlung imaging can effectively monitor the 32 P sustained‐release seeds and their in vivo biodistribution and lays a foundation for the sustained‐release seeds prostatic targeted implantation .

Measurement of the photoeffect cross section and the K-absorption edge energy of Dy, Ta, Pt and Au atoms using Bremsstrahlung / Medición de la sección eficaz de fotoefecto y de la energía del borde de absorción K de los átomos Dy, Ta, Pt y Au utilizando radiación de frenado

An experimental setup to determine the K-shell photoelectric cross-section of Dy, Ta, Pt and Au atoms was implemented at the Nuclear Analytical Laboratory (LAN) of the InSTEC. Bremsstrahlung photons, produced by - beta particles hitting a thin Ni converter, were used to irradiate the target under study. A HPGe detector, coupled to standard nuclear instrumentation, collected the incident and transmitted spectra. A sharp decrease in intensity at the K-shell binding energy was observed in the transmitted spectra. The photon beam divergence effects were corrected with a calibration curve calculated with Monte Carlo simulations (MCNPX 2.6). In order to establish accurately the cross section at the K-edge energy, the obtained data was processed by two methods: fitting the total cross section to a sigmoidal function, as well as the cross section branches around the K-edge to the empirical law . The Empirical Law method was introduced in this work to minimize the detector resolution effects. The results were compared with experimental and theoretical values showing the best agreement when the thinner targets were used. For the first time the photoeffect cross section at the K-edge energy for Pt is reported at first time.

Se determina la sección eficaz fotoeléctrica de la capa K de los átomos Dy, Ta, Pt y Au en un arreglo experimental desarrollado en el Laboratorio Analítico Nuclear del InSTEC. Los blancos bajo estudio se irradiaron con fotones de frenado producidos en un radiador de Ni por las partículas beta emitidas por una fuente de -. Los espectros incidentes y de transmisión se colectaron en un detector de germanio hiperpuro, acoplado a su instrumentación nuclear estándar. En los espectros de transmisión se observó un decrecimiento agudo de la intensidad correspondiente a la energía del borde K. Los efectos de interacciones múltiples del haz fotónico en las láminas blanco se corrigieron a través de una curva de calibración calculada mediante simulaciones Monte Carlo (MCNPX 2.6). Con vistas a garantizar la mejor precisión en la determinación de la sección eficaz para la energía del borde K, los datos obtenidos se ajustaron según dos comportamientos funcionales en esta región: una sigmoide y una ley empírica del tipo . Este último método se introdujo en el trabajo y permite minimizar los efectos resolutivos. Los resultados obtenidos se compararon con valores teóricos y experimentales, mostrando mayor concordancia cuando se emplean blancos finos. Se reporta, por primera vez, la sección eficaz de fotoefecto en el borde K del platino (Pt).