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Feasibility, design and sensitivity studies on innovative nuclear reactors that could address the issue of nuclear waste transmutation using fuels enriched in minor actinides, require high accuracy cross section data for a variety of neutron-induced reactions from thermal energies to several tens of MeV. The isotope 241Am (T1/2= 433 years) is present in high-level nuclear waste (HLW), representing about 1.8 % of the actinide mass in spent PWR UOx fuel. Its importance increases with cooling time due to additional production from the β-decay of 241Pu with a half-life of 14.3 years. The production rate of 241 Am in conventional reactors, including its further accumulation through the decay of 241Pu and its destruction through transmutation/incineration are very important parameters for the design of any recycling solution. In the present work, the 241 Am(n,f) reaction cross-section was measured using Micromegas detectors at the Experimental Area 2 of the n_TOF facility at CERN. For the measurement, the 235U(n,f) and 238U(n,f) reference reactions were used for the determination of the neutron flux. In the present work an overview of the experimental setup and the adopted data analysis techniques is given along with preliminary results.
Inhibitoren der Apoptose (IAP, inhibitor of apoptosis) Proteine spielen eine wichtige Rolle in Bezug auf Zelltodregulation und es ist anzunehmen, dass eine Dysregulation dieser Proteine zu einer Tumorentwicklung und Tumorprogression beiträgt. Erhöhte Expressionslevel von IAP Proteinen verhindern die Aktivierbarkeit des Zelltodprogrammes von Tumorzellen und eine Reihe von Studien konnte bereits erhöhte IAP Level in Tumorzelllinien sowie in primären Tumorproben nachweisen. Des Weiteren korrelieren erhöhte Expressionslevel von IAPs in Tumoren mit Behandlungsresistenzen und schlechten Prognosen für die Patienten.
Das diffuse großzellige B-Zell Lymphom (DLBCL, diffuse large B-cell lymphoma) zählt zu den häufigsten Subtypen der Non-Hodgkin Lymphome (NHL) mit 40 % aller neu diagnostizierten NHL Fälle. DLBCL ist eine sehr heterogene Erkrankung die in drei verschiedene Gruppen klassifiziert wurde: aktivierter B-Zell Typ (ABC, activated B-cell), Keimzentrum B-Zell Typ (GCB, germinal center B-Cell) und Mediastinaler großzelliger B-Zell Typ (PMBL, primary mediastinal B-cell lymphoma). Erhöhte Expressionslevel von zellulärem IAP1 (cIAP, cellular IAP) und cIAP2 wurden ebenfalls in primären Tumorproben von DLBCL Patienten nachgewiesen. Smac mimetics wurden entwickelt, um IAPs zu antagonisieren und stellen damit eine Behandlungsstrategie für DLBCL Patienten dar, denn ca. 40 % aller DLBCL Patienten entwickeln ein Rezidiv oder erreichen gar keine Remission unter Standardtherapie. Jedoch ist der Effekt von Smac mimetics in einer Einzelbehandlung limitiert, weswegen Kombinationstherapien mit Smac mimetics eine vielversprechende Strategie für ihren klinischen Einsatz darstellen. Aus diesem Grund haben wir in dieser Arbeit den Effekt von Smac mimetic in Kombination mit Proteasom-Inhibitoren analysiert und einen speziellen Fokus auf den molekularen Mechanismus des ausgelösten Zelltodsignalweges gelegt.
Die Kombination verschiedener Konzentrationen des Smac mimetics BV6 mit dem Proteasom-Inhibitor carfilzomib (CFZ) löst in allen drei getesteten DLBCL Subtypen (ABC, GCB und PMBL) Zelltod aus. Die Kalkulation des Kombinationsindexes (CI, combination index) sowie des Bliss Scores, zwei quantitative Parameter zur Bestimmung eines Synergismus, zeigen, dass fast alle getesteten Kombinationen einen Synergismus aufweisen. Dies verdeutlicht, dass eine Co-Behandlung von BV6 und CFZ eine wirksame Kombination ist um Zelltod in DLBCL Zelllinien auszulösen. Außerdem zeigt eine Kombination von BV6 mit anderen Proteasom-Inhibitoren wie ixazomib (IXA) oder oprozomib (OPR), ebenfalls eine synergistische Reduktion der Zellviabilität. Diese Ergebnisse deuten darauf hin, dass der detektierte Effekt nicht auf eine Substanz limitiert ist, sondern, dass ein genereller Effekt von Smac mimetic und Proteasom-Inhibitoren vorliegt, um Zellviabilität in DLBCL zu reduzieren. BV6 und CFZ induzieren einen apoptotischen Zelltod, da sie die Spaltung und Aktivierung von Initiator- und Effektorcaspasen (Caspasen-3, -7, -8 und -9) initiieren und sich der induzierte Zelltod mit Hilfe des Caspasen-Inhibitors zVAD.fmk verhindern lässt. Die Behandlung mit BV6 und CFZ führt zu einer Akkumulation von NIK, ein Protein welches zur Aktivierung des non-kanonischen NF-kB Signalweges benötigt wird. Weitere Untersuchungen zeigen jedoch, dass NIK nicht an der Zelltodinduktion beteiligt ist, da eine siRNA-basierte Herunterregulierung des NIK Proteins keinen Einfluss auf die Zelltodinduktion nimmt. Ebenfalls ist der Zelltod unabhängig von dem TNFa Signalweg, da weder eine Behandlung mit dem TNFa Inhibitor Enbrel den Zelltod verringern kann noch eine zusätzliche Gabe von TNFa den Zelltod erhöht. Weitere mechanistische Studien zeigen eine kritische Rolle der mitochondrialen Apoptose für den BV6/CFZ-vermittelten Zelltod. Unter Behandlung mit BV6/CFZ wurde eine Aktivierung von BAX und BAK nachgewiesen, welche beide mit verantwortlich für die Porenbildung in der mitochondrialen Membran sind. Eine Herunterregulation dieser beiden Proteine mittels siRNA reduziert signifikant den durch BV6/CFZ-induzierten Zelltod auf ein Minimum. Gleichzeitig löst eine Co-Behandlung mit BV6/CFZ einen Verlust des mitochondrialen Membranpotentials (LOMMP, loss of mitochondrial membrane potential) aus. In Übereinstimmung mit den vorherigen Experimenten, zeigen wir eine Akkumulation von mitochondrialen reaktiven Sauerstoffspezies (ROS; reactive oxygen species), sowie einen generellen Anstieg des allgemeinen ROS Levels. Eine Behandlung mit BV6/CFZ zeigt eine deutliche Akkumulation des pro-apoptotischen Proteins NOXA. Um dessen funktionelle Relevanz zu überprüfen, wurde die Proteinmenge von NOXA mittels siRNA stark reduziert. Eine Behandlung mit der Kombination aus BV6 und CFZ zeigt daraufhin eine signifikant reduzierte Zelltodinduktion, was die funktionelle Relevanz von NOXA für den BV6/CFZ-vermittelten Zelltod unterstreicht. Immunopräzipitationsstudien zeigen, dass in RIVA und U2932 Zellen NOXA konstitutiv an seinen anti-apoptotischen Bindungspartner MCL-1 gebunden ist, was die Zellen bereits darauf vorbereitet Apoptose zu durchlaufen. Dieses sogenannte „primen“ für Apoptose wird durch die Behandlung mit BV6 und CFZ weiter verstärkt, da es die Bindung zwischen NOXA und MCL-1 weiter erhöht. Dadurch wird die Balance zwischen pro- und anti-apoptotischen Proteinen zu Gunsten der pro-apoptotischen Proteine verschoben und die Induktion von Apoptose begünstigt.
Insgesamt zeigen die Ergebnisse, dass DLBCL Zelllinien sensitiv auf eine Behandlung mit Smac mimetic und Proteasom-Inhibitor reagieren und damit eine mögliche neue Behandlungsstrategie für diese heterogene Tumorerkrankung darstellt.
Neutron total cross sections are an important source of experimental data in the evaluation of neutron-induced cross sections. The sum of all neutron-induced reaction cross sections can be determined with a precision of a few per cent in a relative measurement. The neutron spectrum of the photoneutron source nELBE extends in the fast region from about 100 keV to 10 MeV and has favourable conditions for transmission measurements due to the low instantaneous flux of neutrons and low gamma-flash background. Several materials of interest (in part included in the CIELO evaluation or on the HPRL of OECD/NEA) have been investigated: 197Au [1, 2], natFe [2], natW [2], 238U, natPt, 4He, natO, natNe, natXe. For gaseous targets high pressure gas cells with flat end-caps have been built that hold up to 200 bar pressure. The experimental setup will be presented including results from several transmission experiments and the data analysis leading to the total cross sections will be discussed.
An accurate measurement of the 140Ce(n,γ) energy-dependent cross-section was performed at the n_TOF facility at CERN. This cross-section is of great importance because it represents a bottleneck for the s-process nucleosynthesis and determines to a large extent the cerium abundance in stars. The measurement was motivated by the significant difference between the cerium abundance measured in globular clusters and the value predicted by theoretical stellar models. This discrepancy can be ascribed to an overestimation of the 140Ce capture cross-section due to a lack of accurate nuclear data. For this measurement, we used a sample of cerium oxide enriched in 140Ce to 99.4%. The experimental apparatus consisted of four deuterated benzene liquid scintillator detectors, which allowed us to overcome the difficulties present in the previous measurements, thanks to their very low neutron sensitivity. The accurate analysis of the p-wave resonances and the calculation of their average parameters are fundamental to improve the evaluation of the 140Ce Maxwellian-averaged cross-section.
Neutron capture on 241Am plays an important role in the nuclear energy production and also provides valuable information for the improvement of nuclear models and the statistical interpretation of the nuclear properties. A new experiment to measure the 241Am(n, γ) cross section in the thermal region and the first few resonances below 10 eV has been carried out at EAR2 of the n_TOF facility at CERN. Three neutron-insensitive C6D6 detectors have been used to measure the neutron-capture gamma cascade as a function of the neutron time of flight, and then deduce the neutron capture yield. Preliminary results will be presented and compared with previously obtained results at the same facility in EAR1. In EAR1 the gamma-ray background at thermal energies was about 90% of the signal while in EAR2 is up to a 25 factor much more favorable signal to noise ratio. We also extended the low energy limit down to subthermal energies. This measurement will allow a comparison with neutron capture measurements conducted at reactors and using a different experimental technique.
Since the start of its operation in 2001, based on an idea of Prof. Carlo Rubbia [1], the neutron time of-flight facility of CERN, n_TOF, has become one of the most forefront neutron facilities in the world for wide-energy spectrum neutron cross section measurements. Thanks to the combination of excellent neutron energy resolution and high instantaneous neutron flux available in the two experimental areas, the second of which has been constructed in 2014, n_TOF is providing a wealth of new data on neutron-induced reactions of interest for nuclear astrophysics, advanced nuclear technologies and medical applications. The unique features of the facility will continue to be exploited in the future, to perform challenging new measurements addressing the still open issues and long-standing quests in the field of neutron physics. In this document the main characteristics of the n_TOF facility and their relevance for neutron studies in the different areas of research will be outlined, addressing the possible future contribution of n_TOF in the fields of nuclear astrophysics, nuclear technologies and medical applications. In addition, the future perspectives of the facility will be described including the upgrade of the spallation target, the setup of an imaging installation and the construction of a new irradiation area.
The neutron capture cross section of 154Gd was measured from 1 eV to 300 keV in the experimental area located 185 m from the CERN n_TOF neutron spallation source, using a metallic sample of gadolinium, enriched to 67% in 154Gd. The capture measurement, performed with four C6D6 scintillation detectors, has been complemented by a transmission measurement performed at the GELINA time-of-flight facility (JRC-Geel), thus minimising the uncertainty related to sample composition. An accurate Maxwellian averaged capture cross section (MACS) was deduced over the temperature range of interest for s process nucleosynthesis modelling. We report a value of 880(50) mb for the MACS at kT = 30 keV, significantly lower compared to values available in literature. The new adopted 154Gd(n,γ) cross section reduces the discrepancy between observed and calculated solar s-only isotopic abundances predicted by s-process nucleosynthesis models.
Setup for the measurement of the 235U(n,f) cross section relative to n-p scattering up to 1 GeV
(2020)
The neutron induced fission of 235U is extensively used as a reference for neutron fluence measurements in various applications, ranging from the investigation of the biological effectiveness of high energy neutrons, to the measurement of high energy neutron cross sections of relevance for accelerator driven nuclear systems. Despite its widespread use, no data exist on neutron induced fission of 235U above 200 MeV. The neutron facility n_TOF offers the possibility to improve the situation. The measurement of 235U(n,f) relative to the differential n-p scattering cross-section, was carried out in September 2018 with the aim of providing accurate and precise cross section data in the energy range from 10 MeV up to 1 GeV. In such measurements, Recoil Proton Telescopes (RPTs) are used to measure the neutron flux while the fission events are detected and counted with dedicated detectors. In this paper the measurement campaign and the experimental set-up are illustrated.
The study of neutron-induced reactions on actinides is of considerable importance for the design of advanced nuclear systems and alternative fuel cycles. Specifically, 230Th is produced from the α-decay of 234U as a byproduct of the 232Th/233U fuel cycle, thus the accurate knowledge of its fission cross section is strongly required. However, few experimental datasets exist in literature with large deviations among them, covering the energy range between 0.2 to 25 MeV. In addition, the study of the 230Th(n,f) cross-section is of great interest in the research on the fission process related to the structure of the fission barriers. Previous measurements have revealed a large resonance at En=715 keV and additional fine structures, but with high discrepancies among the cross-section values of these measurements. This contribution presents preliminary results of the 230Th(n,f) cross-section measurements at the CERN n_TOF facility. The high purity targets of the natural, but very rare isotope 230Th, were produced at JRC-Geel in Belgium. The measurements were performed at both experimental areas (EAR-1 and EAR-2) of the n_TOF facility, covering a very broad energy range from thermal up to at least 100 MeV. The experimental setup was based on Micromegas detectors with the 235U(n,f) and 238U(n,f) reaction cross-sections used as reference.