Zugl.: Zürich, Universiẗat, Diss., 2004.

1. A quantitive understanding of the nucleosynthesis process requires the knowledge of the production rates, the masses and the ?-decay characteristics of exotic neutron-rich nu- clei. Nuclear fission is a suitable method of producing such nuclei with masses from 60 - 150. Neutron-rich nuclei close to the r-process path can be produced via photo-fission at the Rossendorf superconducting linear accelerator of high brilliance and low emittance (ELBE) or by means of nuclear reactions at relativistic energies (for example at GSI). If the fission prod- ucts are identified and also their charge numbers are obtained, it will be principally possible to investigate their structure by means of beta-gamma spectroscopy. 2. For the purpose of fission-fragment detection a double time-of-flight (TOF) spectrometer has been developed. The key component of the TOF spectrometer is a TOF detector consisting of multichannel-plate (MCP) detectors with a position-sensitive readout, a foil for secondary electron (SE) production and an electrostatic mirror. The fission fragments are detected by measuring the SEs impinging on the position-sensitive anode after emission from the foil, ac- celeration and deflection by the electrostatic mirror. 3. In the first part of the work, special attention is paid to the relevant methods of building a spectrometer of such type. The functionality of the different detector components is proven in detail. A unique method for the determination of the SE foil thickness with ?-particles is pre- sented. Values for the mirror transmission and scattering are deduced. A dedicated SIMION 3D simulation showed that introducing serpentine like wires with pitch distance of 1 mm is capable of providing transparency of more than 90% without significant impact on the time resolution. 4. Since the performance of the MCP detectors is crucial, optimised schemes for their high- voltage supplies have been implemented successfully. Further enhancement of the setup was achieved by introducing surface-mount device (SMD) elements for signal decoupling, positioned close to the detector surface. Thus, we succeeded in avoiding signal deterioration coming from the additional capacitances and inductivities caused by extra cable lengths. Because the MCP signal decoupling takes place by means of rings with not well-defined impedance, impedance- matching problems arise, causing signal ringing and distortion. An approach towards solving this problem was to build a special fast, wide-band transimpedance amplifier. Using its circuit mounted close to the detectors, a significant reduction of the signal ringing was observed while maintaining the rise time of the detector signal. In order to process the multichannel-plate de- tector signals optimally, a new state-of-the-art constant-fraction discriminator (CFD) based on the amplitude and rise time compensated (ARC) technique with very low threshold capabilities and optimised walk properties has been developed and incorporated into the setup. 5. In our first laboratory test measurements conducted with an ?-particle source, we demonstrated ability of the setup to resolve pattern images placed directly in front of the MCP detector or reflected by the electrostatic mirror. The obtained position resolution for the second case is in the order of 2 mm. We showed that the detection efficiency of the system for ions like He is less than 30 %. This is mainly due to the low number of the electrons liberated from the SE foil. In a setup consisting of two mirror MCP detectors, we could successfully observe the TOF spectrum of a mixed (226Ra, 222Rn, 210Po, 218Po, 214Po) ?-source and found a good agreement with a SRIM simulation. 6. Measurements performed at the FZ Dresden-Rossendorf 5 MV tandem accelerator en- abled us to learn more about the response of the TOF detectors to various beams of heavy ions. The first in-beam experiments clearly showed that the applied setup consisting of two mirror detectors is capable of resolving different 35Cl beam charge states. In a combination with the specially designed wide-band amplifier and dedicated CFDs based on the ARC technique, we managed to achieve an in-beam time resolution of 170 ps per TOF detector. Measurements with ions of Z > 30 resulted in detection efficiencies of greater than 90%. At foil accelerating potentials approximately two times larger than the mirror deflection voltage, most of the SEs gain enough energy to pass through the electrostatic mirror without being deflected towards the MCP surface. Thus, an abrupt drop of the efficiency curve was observed - the “transparent” mode of the mirror. 7. Properties of electrons ejected from thin foils from heavy ions have been also investigated. From the MCP pulse-height-distribution spectra, a number for the forward-emitted SEs ejected by 35Cl beam was deduced. A method for obtaining widths of the SE energy distributions from the drop of the efficiency curve for various ions has been proposed. Assuming that the efficiency curve as a function of the accelerating voltage follows an error function, its standard deviation gives the standard deviation of the SE energy distribution. Another method based on the TOF technique for reconstructing the secondary electron velocity and energy distribution was also invented. It was found that the resulting mean SE velocity closely approaches the one of the beam ions. This phenomenon was attributed to the so-called “convoy” electrons. 8. The obtained position resolution for beams like 35Cl, 79Br and 107Ag at stable detection efficiency was better than 1.8 mm. It was demonstrated that with increasing the foil accelerat- ing voltage, the position resolution improves due to the minimised SE angular spread. Such a mode of operation was favoured until the mirror “semi-transparency” regime was reached, after which increasing further the accelerating potential could lead to a position resolution worsen- ing. An explanation of the fact could be the deterioration of the anode timing signals or some defocusing effects arising from the mirror wires field at high accelerating voltages. 9. Testing photo-fission experiments were performed at the bremsstrahlung facility at the ELBE accelerator. For the first time a spectrometer of this kind was successfully employed for bremsstrahlung-induced photo-fission measurements. The setup consisted of two mirror detectors (first arm) and a 80 mm diameter MCP detector (second arm) with a 238U target positioned in between. TOF measurements with two bremsstrahlung end-point energies of 12.9 and 16.0 MeV were carried out. A clear cut separation of the TOF peaks for the medium- mass and heavy fission fragments was observed. At these experimental test runs, we did not aim at one-by-one fission fragment mass resolution, since this may be the purpose of a more specific experiment utilising a much thinner fissile source than the one applied here (minimum straggling of the fragments inside the target is required) and considerably better statistics. It was possible to estimate the photo-fission production rate for the two measuring cases and to compare the obtained results with data from other measurements.

Zugl.: Trier, Univ., Diss., 2006

Zugl.: Augsburg, Univ., Diss., 2006 u.d.T.: Haseloff, Anikar Michael: Public network access points und der digital divide

1. A quantitive understanding of the nucleosynthesis process requires the knowledge of the production rates, the masses and the ?-decay characteristics of exotic neutron-rich nu- clei. Nuclear fission is a suitable method of producing such nuclei with masses from 60 - 150. Neutron-rich nuclei close to the r-process path can be produced via photo-fission at the Rossendorf superconducting linear accelerator of high brilliance and low emittance (ELBE) or by means of nuclear reactions at relativistic energies (for example at GSI). If the fission prod- ucts are identified and also their charge numbers are obtained, it will be principally possible to investigate their structure by means of beta-gamma spectroscopy. 2. For the purpose of fission-fragment detection a double time-of-flight (TOF) spectrometer has been developed. The key component of the TOF spectrometer is a TOF detector consisting of multichannel-plate (MCP) detectors with a position-sensitive readout, a foil for secondary electron (SE) production and an electrostatic mirror. The fission fragments are detected by measuring the SEs impinging on the position-sensitive anode after emission from the foil, ac- celeration and deflection by the electrostatic mirror. 3. In the first part of the work, special attention is paid to the relevant methods of building a spectrometer of such type. The functionality of the different detector components is proven in detail. A unique method for the determination of the SE foil thickness with ?-particles is pre- sented. Values for the mirror transmission and scattering are deduced. A dedicated SIMION 3D simulation showed that introducing serpentine like wires with pitch distance of 1 mm is capable of providing transparency of more than 90% without significant impact on the time resolution. 4. Since the performance of the MCP detectors is crucial, optimised schemes for their high- voltage supplies have been implemented successfully. Further enhancement of the setup was achieved by introducing surface-mount device (SMD) elements for signal decoupling, positioned close to the detector surface. Thus, we succeeded in avoiding signal deterioration coming from the additional capacitances and inductivities caused by extra cable lengths. Because the MCP signal decoupling takes place by means of rings with not well-defined impedance, impedance- matching problems arise, causing signal ringing and distortion. An approach towards solving this problem was to build a special fast, wide-band transimpedance amplifier. Using its circuit mounted close to the detectors, a significant reduction of the signal ringing was observed while maintaining the rise time of the detector signal. In order to process the multichannel-plate de- tector signals optimally, a new state-of-the-art constant-fraction discriminator (CFD) based on the amplitude and rise time compensated (ARC) technique with very low threshold capabilities and optimised walk properties has been developed and incorporated into the setup. 5. In our first laboratory test measurements conducted with an ?-particle source, we demonstrated ability of the setup to resolve pattern images placed directly in front of the MCP detector or reflected by the electrostatic mirror. The obtained position resolution for the second case is in the order of 2 mm. We showed that the detection efficiency of the system for ions like He is less than 30 %. This is mainly due to the low number of the electrons liberated from the SE foil. In a setup consisting of two mirror MCP detectors, we could successfully observe the TOF spectrum of a mixed (226Ra, 222Rn, 210Po, 218Po, 214Po) ?-source and found a good agreement with a SRIM simulation. 6. Measurements performed at the FZ Dresden-Rossendorf 5 MV tandem accelerator en- abled us to learn more about the response of the TOF detectors to various beams of heavy ions. The first in-beam experiments clearly showed that the applied setup consisting of two mirror detectors is capable of resolving different 35Cl beam charge states. In a combination with the specially designed wide-band amplifier and dedicated CFDs based on the ARC technique, we managed to achieve an in-beam time resolution of 170 ps per TOF detector. Measurements with ions of Z > 30 resulted in detection efficiencies of greater than 90%. At foil accelerating potentials approximately two times larger than the mirror deflection voltage, most of the SEs gain enough energy to pass through the electrostatic mirror without being deflected towards the MCP surface. Thus, an abrupt drop of the efficiency curve was observed - the “transparent” mode of the mirror. 7. Properties of electrons ejected from thin foils from heavy ions have been also investigated. From the MCP pulse-height-distribution spectra, a number for the forward-emitted SEs ejected by 35Cl beam was deduced. A method for obtaining widths of the SE energy distributions from the drop of the efficiency curve for various ions has been proposed. Assuming that the efficiency curve as a function of the accelerating voltage follows an error function, its standard deviation gives the standard deviation of the SE energy distribution. Another method based on the TOF technique for reconstructing the secondary electron velocity and energy distribution was also invented. It was found that the resulting mean SE velocity closely approaches the one of the beam ions. This phenomenon was attributed to the so-called “convoy” electrons. 8. The obtained position resolution for beams like 35Cl, 79Br and 107Ag at stable detection efficiency was better than 1.8 mm. It was demonstrated that with increasing the foil accelerat- ing voltage, the position resolution improves due to the minimised SE angular spread. Such a mode of operation was favoured until the mirror “semi-transparency” regime was reached, after which increasing further the accelerating potential could lead to a position resolution worsen- ing. An explanation of the fact could be the deterioration of the anode timing signals or some defocusing effects arising from the mirror wires field at high accelerating voltages. 9. Testing photo-fission experiments were performed at the bremsstrahlung facility at the ELBE accelerator. For the first time a spectrometer of this kind was successfully employed for bremsstrahlung-induced photo-fission measurements. The setup consisted of two mirror detectors (first arm) and a 80 mm diameter MCP detector (second arm) with a 238U target positioned in between. TOF measurements with two bremsstrahlung end-point energies of 12.9 and 16.0 MeV were carried out. A clear cut separation of the TOF peaks for the medium- mass and heavy fission fragments was observed. At these experimental test runs, we did not aim at one-by-one fission fragment mass resolution, since this may be the purpose of a more specific experiment utilising a much thinner fissile source than the one applied here (minimum straggling of the fragments inside the target is required) and considerably better statistics. It was possible to estimate the photo-fission production rate for the two measuring cases and to compare the obtained results with data from other measurements.

Dès notre prise de fonction dans un service hospitalier qui a accueilli des patients infectés par le V.l.H., nous nous sommes demandées si l'intervention psychologique était possible dans ce lieu hautement spécialisé ? Avec l'éloignement du caractère mortel de la maladie,le V.l.H. prend davantage le sens d'une maladie chronique. Les limites reculent mais à quel prix ? La dernière partie de cette recherche propose une réflexion psychopathologique et psychanalytique sur les problèmes posés par la "poussée" à la mort et que nous avons vu se déchaîner dans cette maladie à travers certaines contaminations volontaires. / When we first started practicing in a hospital unitth at treated V.l.H. positive patients, we asked ourselve:in the fîrst part of this research, if psychological intervention was possible in such a highly specialized unit. With the receding of te deadly nature of Aids, it appears more a chronic illness. The limîts are pushed back, but at what price ? Finally, the part of this research proposes a psychopathological reflection on the problems posed by the"death drive" présent at the very heart of the drive, and that we've seen un leashed by this pathologyby the act of intentional contaminations.

No description available.

Präzise neutroneninduzierte Spaltquerschnitte von Actinoiden wie den Plutoniumisotopen haben für die Entwicklung zukünftiger Transmutationstechnologien eine große Bedeutung. Die Unsicherheiten des Pu(242)-Spaltquerschnitts im schnellen Bereich des Spektrums betragen derzeit etwa 21 %. Aktuelle Sensitivitätsstudien haben gezeigt, dass nur eine Reduzierung dieser Unsicherheiten auf unter 5% verlässliche neutronenphysikalische Simulationen zulässt. Diese anspruchsvolle Aufgabe konnte im Rahmen der vorliegenden Arbeit an der Neutronenfugzeitanlage nELBE durchgeführt werden. Dünne, homogene und großfächige Actinoiden-Proben wurden dem Helmholtz-Zentrum Dresden-Rossendorf innerhalb des TRAKULA-Verbundprojektes zur Verfügung gestellt. Eingesetzt in eine neu entwickelte Spaltionisationskammer ermöglichten sie eine akkurate Bestimmung des Pu(242)- Spaltquerschnitts relativ zu U(235). Die Flächendichten der Plutoniumschichten wurden anhand der spontanen Spaltrate von Pu(242) bestimmt. Aufwändige Teilchentransportsimulationen (durchgeführt mit Geant 4, MCNP 6 und FLUKA) wurden genutzt, um die auftretende Neutronenstreuung zu korrigieren. Die gewonnenen Ergebnisse sind im Rahmen ihrer Unsicherheiten in guter Übereinstimmung mit aktuellen Kerndatenevaluierungen. / Neutron induced fssion cross sections of actinides like the Pu-isotopes are of relevance for the development of nuclear transmutation technologies. For Pu(242), current uncertainties are of around 21%. Sensitivity studies show that the total uncertainty has to be reduced to below 5% to allow for reliable neutron physics simulations. This challenging task was performed at the neutron time-of-fight facility of the new German National Center for High Power Radiation Sources at HZDR, Dresden. Within the TRAKULA project, thin, large and homogeneous deposits of U(235) and Pu(242) have been produced successfully. Using two consecutively placed fssion chambers allowed the determination of the neutron induced fssion cross section of Pu(242) relative to U(235). The areal density of the Plutonium targets was calculated using the measured spontaneous fssion rate. Experimental results of the fast neutron induced fssion of Pu(242) acquired at nELBE will be presented and compared to recent experiments and evaluated data. Corrections addressing the neutron scattering are discussed by using results of different neutron transport simulations (Geant 4, MCNP 6 and FLUKA).

Präzise neutroneninduzierte Spaltquerschnitte von Actinoiden wie den Plutoniumisotopen haben für die Entwicklung zukünftiger Transmutationstechnologien eine große Bedeutung. Die Unsicherheiten des Pu(242)-Spaltquerschnitts im schnellen Bereich des Spektrums betragen derzeit etwa 21 %. Aktuelle Sensitivitätsstudien haben gezeigt, dass nur eine Reduzierung dieser Unsicherheiten auf unter 5% verlässliche neutronenphysikalische Simulationen zulässt. Diese anspruchsvolle Aufgabe konnte im Rahmen der vorliegenden Arbeit an der Neutronenfugzeitanlage nELBE durchgeführt werden. Dünne, homogene und großfächige Actinoiden-Proben wurden dem Helmholtz-Zentrum Dresden-Rossendorf innerhalb des TRAKULA-Verbundprojektes zur Verfügung gestellt. Eingesetzt in eine neu entwickelte Spaltionisationskammer ermöglichten sie eine akkurate Bestimmung des Pu(242)- Spaltquerschnitts relativ zu U(235). Die Flächendichten der Plutoniumschichten wurden anhand der spontanen Spaltrate von Pu(242) bestimmt. Aufwändige Teilchentransportsimulationen (durchgeführt mit Geant 4, MCNP 6 und FLUKA) wurden genutzt, um die auftretende Neutronenstreuung zu korrigieren. Die gewonnenen Ergebnisse sind im Rahmen ihrer Unsicherheiten in guter Übereinstimmung mit aktuellen Kerndatenevaluierungen.:1 Einleitung 1.1 Partitionierung und Transmutation 1.2 Die Bedeutung von Pu(242) für P&T 1.3 Bisherige Experimente 1.4 Evaluierungen 1.5 Gliederung dieser Arbeit 2 Spaltwahrscheinlichkeit 2.1 Statistisches Modell und Compoundkern 2.2 Kernreaktionsrechnungen 3 Die Neutronenfugzeitanlage nELBE 4 Spaltionisationskammern 4.1 Die nELBE Spaltkammern 4.1.1 Actinoidenschichten 4.1.2 Aufbau 4.1.3 Gasversorgung 4.1.4 Optimierung des elektrischen Feldes 4.1.5 Simulationen von Impulshöhenverteilungen 4.2 Die PTB U(235) Spaltkammer H19 5 Experimente zur Spaltung von Pu(242) 5.1 Experimentelle Bestimmung neutroneninduzierter Spaltquerschnitte 5.2 Messaufbau 5.3 Datenaufnahme und -verarbeitung 5.4 Datenanalyse 5.4.1 Bestimmung der Spontanspaltrate 5.4.2 Bestimmung des neutroneninduzierten Spaltquerschnitts von Pu(242) 5.5 Ergebnisse und Diskussion 5.5.1 Diskussion 5.5.2 Unsicherheiten 5.5.3 Vergleich mit Kernreaktionsrechnungen 6 Zusammenfassung und Ausblick Anhang A.1 Depositionszelle A.2 Neutronenfugzeitanlagen A.3 Spaltfragmentverteilungen mit GEF A.4 Experimenteller Aufbau A.5 Aufbau der Datenaufnahme/-verarbeitung A.5.1 Verwendete Elektronik A.6 Stabilität der Datenaufnahme A.7 Konsistenzbetrachtung der Querschnittsbestimmung Literaturverzeichnis Abbildungsverzeichnis Tabellenverzeichnis Liste der verwendeten Akronyme Publikationen / Neutron induced fssion cross sections of actinides like the Pu-isotopes are of relevance for the development of nuclear transmutation technologies. For Pu(242), current uncertainties are of around 21%. Sensitivity studies show that the total uncertainty has to be reduced to below 5% to allow for reliable neutron physics simulations. This challenging task was performed at the neutron time-of-fight facility of the new German National Center for High Power Radiation Sources at HZDR, Dresden. Within the TRAKULA project, thin, large and homogeneous deposits of U(235) and Pu(242) have been produced successfully. Using two consecutively placed fssion chambers allowed the determination of the neutron induced fssion cross section of Pu(242) relative to U(235). The areal density of the Plutonium targets was calculated using the measured spontaneous fssion rate. Experimental results of the fast neutron induced fssion of Pu(242) acquired at nELBE will be presented and compared to recent experiments and evaluated data. Corrections addressing the neutron scattering are discussed by using results of different neutron transport simulations (Geant 4, MCNP 6 and FLUKA).:1 Einleitung 1.1 Partitionierung und Transmutation 1.2 Die Bedeutung von Pu(242) für P&T 1.3 Bisherige Experimente 1.4 Evaluierungen 1.5 Gliederung dieser Arbeit 2 Spaltwahrscheinlichkeit 2.1 Statistisches Modell und Compoundkern 2.2 Kernreaktionsrechnungen 3 Die Neutronenfugzeitanlage nELBE 4 Spaltionisationskammern 4.1 Die nELBE Spaltkammern 4.1.1 Actinoidenschichten 4.1.2 Aufbau 4.1.3 Gasversorgung 4.1.4 Optimierung des elektrischen Feldes 4.1.5 Simulationen von Impulshöhenverteilungen 4.2 Die PTB U(235) Spaltkammer H19 5 Experimente zur Spaltung von Pu(242) 5.1 Experimentelle Bestimmung neutroneninduzierter Spaltquerschnitte 5.2 Messaufbau 5.3 Datenaufnahme und -verarbeitung 5.4 Datenanalyse 5.4.1 Bestimmung der Spontanspaltrate 5.4.2 Bestimmung des neutroneninduzierten Spaltquerschnitts von Pu(242) 5.5 Ergebnisse und Diskussion 5.5.1 Diskussion 5.5.2 Unsicherheiten 5.5.3 Vergleich mit Kernreaktionsrechnungen 6 Zusammenfassung und Ausblick Anhang A.1 Depositionszelle A.2 Neutronenfugzeitanlagen A.3 Spaltfragmentverteilungen mit GEF A.4 Experimenteller Aufbau A.5 Aufbau der Datenaufnahme/-verarbeitung A.5.1 Verwendete Elektronik A.6 Stabilität der Datenaufnahme A.7 Konsistenzbetrachtung der Querschnittsbestimmung Literaturverzeichnis Abbildungsverzeichnis Tabellenverzeichnis Liste der verwendeten Akronyme Publikationen

Die Verpackung und Spaltung konkatemerer DNA ist ein essentieller Prozeß bei der Reifung von Virionen. Die an diesem Prozess maßgeblich beteiligten Proteine werden als Terminase bezeichnet. Die Inhibition der HCMV Terminase bietet einen attraktiven alternativen Ansatzpunkt für die antivirale Therapie. Zur Inhibition der Terminase Aktivität wurden die neuen Benzimidazol D-Ribonukleosid Derivate BTCRB und Cl4RB auf ihre antivirale Wirkung analysiert. Die neuen Benzimidazol D-Ribonukleosid Derivate BTCRB und Cl4RB zeigten sowohl gegen den HCMV Laborstamm AD169 als auch gegen klinische HCMV-Isolaten eine Wirkung. Weiterhin wurde die Wirksamkeit der Substanzen auf anderen Herpesviren getestet. Interessanterweise zeigten BTCRB und Cl4RB sowohl einen Effekt gegen Varicella-Zoster-Virus (VZV) als auch Ratten-Cytomegalovirus (RCMV), wohingegen der Effekt gegen Herpes-simplex-Virus Typ-1 (HSV-1) und Maus-Cytomegalovirus (MCMV) gering war. Infolgedessen eignen sich beide Substanzen BTCRB und Cl4RB als attraktive alternative Inhibitoren für die weitere Entwicklung einer antiviralen Therapie. / DNA packaging is the key step in viral maturation and involves binding and cleavage of viral DNA containing specific DNA-packaging motifs. This process is mediated by a group of specific enzymes called terminase. The development for an inhibitor of HCMV terminase would be of great value, because it would act subsequent to DNA synthesis and block the first steps in viral maturation. Therefore we characterized two inhibitors targeting the HCMV terminase, 2-bromo-4,5,6-trichloro-1-(2,3,5-tri-O-acetly-ß-D-ribofuranosyl) benzimidazole (BTCRB) and 2,4,5,6-tetrachloro-1-(2,3,5-tri-O-acetly-ß-D-ribofuranosyl) benzimidazole (Cl4RB). By using viral plaque formation, viral yield, viral growth kinetics and electron microscopy, we demonstrated that two compounds BTCRB und Cl4RB are highly active against HCMV AD 169 and HCMV clinical isolates. In addition, the antiviral effect on other herpesviruses was determined. Interestingly BTCRB was active all tested herpesviruses. The best effects were observed on VZV-and RCMV-infected cells. Therefore new compounds might be promising attractive compounds for antiviral therapy in the future.