Despite nuclear fission prominence in nuclear physics, there are still several fundamental open questions about this process. One uncertainty is the energy distribution of neutrons emitted immediately after fission. In particular the relative energy distribution of neutrons above 8~MeV has been difficult to measure. This experiment measured the prompt neutron energy spectrum of n+235U from 3-10~MeV. The measurement took place at Los Alamos National Laboratory (LANL) and used a double time-of-flight technique to measure both the beam and fission neutron kinetic energies. Fission event timing was measured with a parallel plate avalanche counter. The fission neutron time-of-flight was measured with 2~m long plastic scintillation detectors. By combining the time-of-flight information with a known flight path the kinetic energy spectrum of neutrons was measured. To eliminate backgrounds various time-of-flight and energy cuts were imposed and an accidental coincidence background was subtracted. An MCNP simulation, including the 2~m neutron detector geometry, was done using the Madland and Nix model as the input energy distribution for the simulated neutrons. Finally, the measured energy spectrum was compared with the MCNP simulated n+235U fission neutron energy spectrum.

A heavily filtered fast neutron irradiation system (FNIS) was developed for a variety of applications, including the study of long-term health effects of fast neutrons by evaluating the biological mechanisms of damage in cultured cells and living animals such as rats or mice. This irradiation system includes an exposure cave made with a lead-bismuth alloy, a cave positioning system, a gamma and neutron monitoring system, a sample transfer system, and interchangeable filters. This system was installed in the irradiation cell of the Texas A&M University Nuclear Science Center Reactor (NSCR). By increasing the thickness of the lead-bismuth alloy, the neutron spectra were shifted into lower energies by the scattering interactions of fast neutrons with the alloy. It is possible, therefore, by changing the alloy thickness, to produce distinctly different dose weighted neutron spectra inside the exposure cave of the FNIS. The calculated neutron spectra showed close agreement with the results of activation foil measurements, unfolded by SAND-II close to the cell window. However, there was a considerable less agreement for locations far away from the cell window. Even though the magnitude of values such as neutron flux and tissue kerma rates in air differed, the weighted average neutron energies showed close agreement between the MCNP and SAND-II since the normalized neutron spectra were in a good agreement each other. A paired ion chamber system was constructed, one with a tissue equivalent plastic (A-150) and propane gas for total dose monitoring, and another with graphite and argon for photon dose monitoring. Using the pair of detectors, the neutron to gamma ratio can be inferred. With the 20 cm-thick FNIS, the absorbed dose rates of neutrons measured with the paired ion chamber method and calculated with the SAND-II results were 13.7 ?? 0.02 Gy/min and 15.5 Gy/min, respectively. The absorbed dose rate of photons and the gamma contribution to total dose were 6.7??10-1 ?? 1.3??10-1 Gy/min and 4.7%, respectively. However, the estimated gamma contribution to total dose varied between 3.6 % to 6.6 % as the assumed neutron sensitivity to the graphite detector was changed from 0.01 to 0.03.

A boron neutron capture enhanced fast neutron therapy assembly has been designed for the Fermilab Neutron Therapy Facility (NTF). This assembly uses a tungsten filter and collimator near the patient¡¯s head, with a graphite reflector surrounding the head to significantly increase the dose due to boron neutron capture reactions. The assembly was designed using Monte Carlo radiation transport code MCNP version 5 for a standard 20x20 cm2 treatment beam. The calculated boron dose enhancement at 5.7-cm depth in a water-filled head phantom in the assembly with a 5x5 cm2 collimation was 21.9% per 100-ppm B-10 for a 5.0-cm tungsten filter and 29.8% for an 8.5-cm tungsten filter. The corresponding dose rate for the 5.0-cm and 8.5-cm thick filters were 0.221 and 0.127 Gy/min, respectively. To validate the design calculations, a simplified BNCEFNT assembly was built using four lead bricks to form a 5x5 cm2 collimator. Five 1.0-cm thick 20x20 cm2 tungsten plates were used to obtain different filter thicknesses and graphite bricks/blocks were used to form a reflector. Measurements of the dose enhancement of the simplified assembly in a water-filled head phantom were performed using a pair of tissue-equivalent ion chambers. One of the ion chambers is loaded with 1000-ppm natural boron (184-ppm 10B) to measure dose due to boron neutron capture. The measured dose enhancement at 5.0-cm depth in the head phantom for the 5.0-cm thick tungsten filter is (16.6 ¡À 1.8)%, which agrees well with the MCNP simulation of the simplified BNCEFNT assembly, (16.4¡À 0.5)%. The error in the calculated dose enhancement only considers the statistical uncertainties. The total dose rate measured at 5.0-cm depth using the non-borated ion chamber is (0.765 ¡À 0.076) Gy/MU, about 61% of the fast neutron standard dose rate (1.255Gy/MU) at 5.0-cm depth for the standard 10x10 cm2 treatment beam. The increased doses to other organs due to the use of the BNCEFNT assembly were calculated using MCNP5 and a MIRD phantom.

Two measurements have been made, addressing gaps in knowledge for 235U(n,f) and 238U(n,f). The energy distribution for prompt fission neutrons is not well-understood below 1 MeV in 235U(n,f). To measure the 235U(n,f) prompt fission neutron distribution, a pulsed neutron beam at the WNR facility in Los Alamos National Laboratory was directed onto a 235U target with neutron detectors placed 1 m from the target. These neutron detectors were designed specifically for this experiment and employed a unique geometry of scintillating plastic material that was designed to reject backgrounds. Fission fragments were detected using an avalanche counter. Coincidences between fission fragment production and neutron detector events were analyzed, using a double time-of-flight technique to determine the energy of the prompt fission neutrons. A separate measurement was made, investigating the neutron-induced fission cross section for 238U(n,f). This measurement also used the pulsed neutron beam at the WNR facility. The neutron flux was normalized to the well-known hydrogen standard and the fission rate was observed for beam neutrons in the energy range of 130-300 MeV. Using an extrapolation technique, the energy dependence of the cross section was determined. These new data filled a sparsely populated energy region that was not well-studied and were measured relative to the hydrogen standard, unlike the majority of available data. These data can be used to constrain the fission cross section, which is considered a nuclear reaction standard.

Este trabalho apresenta os resultados dos valores de fluxo de nêutrons obtidos a partir da implantação de uma armadilha de nêutrons no núcleo do Reator IPEN/MB-01. Foram analisadas várias configurações de armadilhas implantadas no núcleo do reator IPEN/MB-01 de forma a se eleger a armadilha mais eficiente. Para a caracterização energética, foram irradiados no centro da armadilha de nêutrons, detetores de ativação de vários materiais diferentes (Au, Sc, In, Ti, Ni). As respectivas espectrometrias gama desses elementos após a irradiação com e sem cobertura de cádmio, forneceram valores experimentais das taxas de reação nuclear (atividade de saturação) por núcleo alvo e as respectivas incertezas que servem de entrada ao código SANDBP que calculou o espectro de energia dos nêutrons no centro do Flux-Trap em 50 grupos de energia, utilizando-se dos espectros de entrada calculados na posição de irradiação (centro do \"Flux Trap\") por códigos de Física de Reatores. Os resultados obtidos constataram um aumento do fluxo de nêutrons térmico no centro da armadilha da configuração 203 em relação a configuração sem armadilha (padrão) da ordem de 350% sem contudo haver a necessidade de se aumentar a potência do reator. Foram também efetuadas comparações entre os espectros desdobrados obtidos pelo SANDBP, em relação aos calculados pelos códigos MCNP-4C e XSDRNPM. A caracterização espacial do fluxo de nêutrons térmicos é feita com folhas de ativação na forma de uma liga infinitamente diluída em massa de 1% de Au e 99% de Al em alguns pontos internos da configuração 203 (axialmente ao Flux Trap\" e adjacências radiais) e os resultados mostraram um aumento significativo da magnitude de seus valores quando comparados a configuração padrão retangular. / This paper presents the results of the neutron flux values obtained from the deployment of a Flux Trap of neutrons in the reactor core IPEN/MB-01. We analyzed several configurations of Flux Traps deployed in the reactor core IPEN/MB-01 in order to get elected to Flux Trap configuration more efficient. To characterize the neutron spectrum were irradiated in the center of the Flux Trap activation detectors of different materials (Au, Sc, In, Ti, Ni). The respective gamma spectroscopy of these elements after irradiation with and without cadmium cover, provided the experimental values of the nuclear reaction rates (saturation activity) by the target nuclei and their uncertainties used as input to the code SANDBP who calculated the energy spectrum of neutrons in the center of the \"Flux-Trap\" in 50 energy groups, using the input spectra calculated at the irradiation position (center of the \"Flux Trap\") by codes for Reactor Physics. The results found an increase in the thermal neutron flux in the center of the Flux Trap configuration 203 for the standard configuration (default) of about 350% without having the need to increase the reactor power. We also made comparisons between the spectra obtained by SANDBP deployed, compared to those calculated by MCNP-4C code and XSDRNPM. The spatial characterization of the thermal neutron flux is made with activation foils in the form of an infinitely dilute bulk alloy of 1% Au and 99% Al in some internal points of the configuration 203 (axially to Flux Trap \"and adjacent radial) and the results showed a significant increase in the magnitude of their values when compared to standard rectangular configuration.

Este trabalho apresenta os resultados dos valores de fluxo de nêutrons obtidos a partir da implantação de uma armadilha de nêutrons no núcleo do Reator IPEN/MB-01. Foram analisadas várias configurações de armadilhas implantadas no núcleo do reator IPEN/MB-01 de forma a se eleger a armadilha mais eficiente. Para a caracterização energética, foram irradiados no centro da armadilha de nêutrons, detetores de ativação de vários materiais diferentes (Au, Sc, In, Ti, Ni). As respectivas espectrometrias gama desses elementos após a irradiação com e sem cobertura de cádmio, forneceram valores experimentais das taxas de reação nuclear (atividade de saturação) por núcleo alvo e as respectivas incertezas que servem de entrada ao código SANDBP que calculou o espectro de energia dos nêutrons no centro do Flux-Trap em 50 grupos de energia, utilizando-se dos espectros de entrada calculados na posição de irradiação (centro do \"Flux Trap\") por códigos de Física de Reatores. Os resultados obtidos constataram um aumento do fluxo de nêutrons térmico no centro da armadilha da configuração 203 em relação a configuração sem armadilha (padrão) da ordem de 350% sem contudo haver a necessidade de se aumentar a potência do reator. Foram também efetuadas comparações entre os espectros desdobrados obtidos pelo SANDBP, em relação aos calculados pelos códigos MCNP-4C e XSDRNPM. A caracterização espacial do fluxo de nêutrons térmicos é feita com folhas de ativação na forma de uma liga infinitamente diluída em massa de 1% de Au e 99% de Al em alguns pontos internos da configuração 203 (axialmente ao Flux Trap\" e adjacências radiais) e os resultados mostraram um aumento significativo da magnitude de seus valores quando comparados a configuração padrão retangular. / This paper presents the results of the neutron flux values obtained from the deployment of a Flux Trap of neutrons in the reactor core IPEN/MB-01. We analyzed several configurations of Flux Traps deployed in the reactor core IPEN/MB-01 in order to get elected to Flux Trap configuration more efficient. To characterize the neutron spectrum were irradiated in the center of the Flux Trap activation detectors of different materials (Au, Sc, In, Ti, Ni). The respective gamma spectroscopy of these elements after irradiation with and without cadmium cover, provided the experimental values of the nuclear reaction rates (saturation activity) by the target nuclei and their uncertainties used as input to the code SANDBP who calculated the energy spectrum of neutrons in the center of the \"Flux-Trap\" in 50 energy groups, using the input spectra calculated at the irradiation position (center of the \"Flux Trap\") by codes for Reactor Physics. The results found an increase in the thermal neutron flux in the center of the Flux Trap configuration 203 for the standard configuration (default) of about 350% without having the need to increase the reactor power. We also made comparisons between the spectra obtained by SANDBP deployed, compared to those calculated by MCNP-4C code and XSDRNPM. The spatial characterization of the thermal neutron flux is made with activation foils in the form of an infinitely dilute bulk alloy of 1% Au and 99% Al in some internal points of the configuration 203 (axially to Flux Trap \"and adjacent radial) and the results showed a significant increase in the magnitude of their values when compared to standard rectangular configuration.

This dissertation focuses on irradiations of a spallation set-up consisting of more than half a ton of natural uranium that were executed by a 660 MeV proton beam at the Joint Institute for Nuclear Reserch in Dubna. Two types of irradiations were arranged: with and without lead shielding. Both types were arranged with threshold activation detectors (Al-27, Mn-55, Co-59, and In-nat) located throughout the whole set-up both in horizontal and vertical positions and activated by secondary neutrons produced by spallation reaction. The threshold activation detectors were analysed by the method of gamma-ray spectroscopy. Radionuclides found in the threshold detectors were analysed and reaction rates were determined for each radionuclide. Ratios of the reaction rates were determined from irradiation of the set-up with and without lead shielding. Subsequently, the neutron spectra generated inside the spallation target at different positions were calculated using Co-59 detector. The experimental results were compared with Monte Carlo simulations performed using MCNPX 2.7.0.

Perhaps surprisingly, the largest experience in operating nuclear power plants has been in nuclear naval propulsion, particularly submarines. This accumulated experience may become the basis of a proposed new generation of compact nuclear power plant designs. In an effort to de-carbonise commercial freight shipping, there is growing interest in the possibility of using nuclear propulsion systems. Reactor cores for such an application would need to be fundamentally different from land-based power generation systems, which require regular refueling, and from reactors used in military submarines, as the fuel used could not conceivably be as highly enriched. Nuclear-powered propulsion would allow ships to operate with low fuel costs, long refueling intervals, and minimal emissions; however, currently such systems remain largely confined to military vessels. This research project undertakes computational modeling of possible soluble-boron-free (SBF) reactor core designs for this application, with a view to informing design decisions in terms of choices of fuel composition, materials, core geometry and layout. Computational modeling using appropriate reactor physics (e.g. WIMS, MONK, Serpent and PANTHER), thermal-hydraulics etc. codes (e.g. COBRA-EN) is used for this project. With an emphasis on reactor physics, this study investigates possible fuel assembly and core designs for civil marine propulsion applications. In particular, it explores the feasibility of using uranium/thorium-rich fuel in a compact, long-life reactor and seek optimal choices and designs of the fuel composition, reactivity control, assembly geometry, and core loading in order to meet the operational needs of a marine propulsion reactor. In this reactor physics and 3D coupled neutronics/thermal-hydraulics study, we attempt to design a civil marine reactor core that fulfills the objective of providing at least 15 effective full-power-years (EFPY) life at 333 MWth. In order to unleash the benefit of thorium in a long life core, the micro-heterogeneous ThO2-UO2 duplex fuel is well-positioned to be utilized in our proposed civil marine core. Unfortunately, A limited number of studies of duplex fuel are available in the public domain, but its use has never been examined in the context of a SBF environment for long-life small modular rector (SMR) core. Therefore, we assumed micro-heterogeneous ThO2-UO2 duplex fuel for our proposed marine core in order to explore its capability. For the proposed civil marine propulsion core design, this study uses 18% U-235 enriched micro-heterogeneous ThO2-UO2 duplex fuel. To provide a basis for comparison we also evaluate the performance of homogeneously mixed 15% U-235 enriched all-UO2 fuel. This research also attempts to design a high power density core with 14 EFPY while satisfying the neutronic and thermal-hydraulics safety constraints. A core with an average power density of 100 MW/m3 has been successfully designed while obtaining a core life of 14 years. The average core power density for this core is increased by ∼50% compared to the reference core design (63 MW/m3 and is equivalent to Sizewell B PWR (101.6 MW/m3 which means capital costs could be significantly reduced and the economic attractiveness of the marine core commensurately improved. In addition, similar to the standard SMR core, a reference core with a power density of 63 MW/m3 has been successfully designed while obtaining a core life of ∼16 years. One of the most important points that can be drawn from these studies is that a duplex fuel lattice needs less burnable absorber than uranium-only fuel to achieve the same poison performance. The higher initial reactivity suppression and relatively smaller reactivity swing of the duplex can make the task of reactivity control through BP design in a thorium-rich core easier. It is also apparent that control rods have greater worth in a duplex core, reducing the control material requirements and thus potentially the cost of the rods. This research also analyzed the feasibility of using thorium-based duplex fuel in different cases and environments to observe whether this fuel consistently exhibit superior performance compared to the UO2 core in both the assembly and whole-core levels. The duplex fuel/core consistently exhibits superior performance in consideration of all the neutronic and TH constraints specified. It can therefore be concluded from this study that the superior performance of the thorium-based micro-heterogeneous ThO2-UO2 duplex fuel provides enhanced confidence that this fuel can be reliably used in high power density and long-life SBF marine propulsion core systems, offering neutronic advantages compared to the all-UO2 fuel. Last, but not least, considering all these factors, duplex fuel can potentially open the avenue for low-enriched uranium (LEU) SBF cores with different configurations. Motivated by growing environmental concerns and anticipated economic pressures, the overall goal of this study is to examine the technological feasibility of expanding the use of nuclear propulsion to civilian maritime shipping and to identify and propose promising candidate core designs.

Das Institut für Kern- und Teilchenphysik (IKTP) der Technischen Universität Dresden (TUD) hat im Forschungszentrum Dresden-Rossendorf (FZD) ein Labor zur Untersuchung von neutroneninduzierten kernphysikalischen Prozessen in Materialien, die für die Fusionsforschung relevant sind, aufgebaut. Das Labor ist ausgestattet mit drei intensiven Neutronenquellen: einer 14 MeV-Neutronenquelle, einer weißen kontinuierlichen Photoneutronen-Quelle, die näher in dieser Arbeit beschrieben wird, und einer gepulsten Photoneutronen-Quelle, die vom FZD inKooperation mit der TUD aufgebaut wurde. Die kontinuierliche Photoneutronen-Quelle basiert auf einem Radiator aus Wolfram (engl. Tungsten Photoneutron Source (TPNS)). TPNS nutzt die im ELBE-Beschleuniger (Elektronen Linearbeschleuniger für Strahlen hoher Brillianz und niedriger Emittanz (ELBE)) beschleunigten Elektronen zur Neutronenerzeugung. Der Prozess läuft über Zwischenschritte ab, indem bei der Abbremsung der Elektronen im Radiator Bremsstrahlungsphotonen entstehen, die anschließend Neutronen durch (γ,xn)-Reaktionen erzeugen. Das Neutronenspektrum der TPNS kann mittels Moderatoren so modifiziert werden, dass es dem in der ersten Wand im Fusionsreaktor entspricht. Dies ermöglicht Untersuchungen mit einem für einen Fusionsreaktor typischen Neutronenspektrum. Die technische Verwirklichung des Projektes, die Inbetriebnahme der Anlage sowie die Durchführung der ersten Experimente zur Neutronenerzeugung ist Inhalt dieser Arbeit. Die Neutronenquelle ist insbesondere für qualitative Untersuchungen in der Fusionsneutronik bestimmt. Der Fusionsreaktor produziert, im Vergleich zu einem Spaltungsreaktor, keine langlebigen Isotope als Abfall. Die wesentliche Aktivität des Reaktors ist in Konstruktionsmaterialien akkumuliert. Durch sorgfältige Auswahl der Materialien kann man die Aktivierung minimieren und damit künftig wesentlich weniger radioaktives Inventar produzieren als in Spaltreaktoren. Ziel der kernphysikalischen Untersuchungen ist, solche Materialien für den Aufbau eines Fusionsreaktors zu erforschen, die niedrigaktivierbar sind, das heißt wenig Aktivität akkumulieren können, und eine Halbwertzeit von einigen Jahren haben. Es ist das Ziel, alle Konstruktionsmaterialien nach 100 Jahren wiederverwenden zu können. Die Neutronenflussdichte einer Photoneutronenquelle ist einige Größenordnungen höher als die, die mittels eines DT-Neutronengenerators mit anschließender Moderation erreicht werden kann. Die gesamte Arbeit ist in drei Teile geteilt. Der erste Teil leitet in die Problematik der Energieversorgung ein und zeigt die Kernfusion als eine vielversprechende Energiequelle der naher Zukunft auf. Das Neutronenlabor der TUD, in dem die TPNS aufgebaut ist, wird ebenfalls kurz vorgestellt. Der zweite Teil befasst sich mit der TPNS selbst, mit ihrem physikalischen Entwurf, der Konstruktion und dem Aufbau bis zu der Inbetriebnahme sowie dem ersten Experiment an der TPNS. Der letzte, dritte Teil ist die Zusammenfassung der vorhandenen Ergebnisse und gibt einen Ausblick auf die zukünftige Vorhaben. / The Institute for Nuclear and Particle Physics at the Technische Universität Dresden (TUD) has build a neutron physics laboratory at Forschungszentrum Dresden-Rossendorf (FZD) to investigate nuclear processes in materials. The experiments are focused on materials relevant to nuclear fusion. The laboratory is equipped with three intensive neutron sources. The first is a 14 MeV monochromatic neutron source based on the DT reaction (owned by TUD); the other two are continuous and pulsed white photoneutron sources based on (γ,xn) reactions. One pulsed photoneutron source is realized by FZD in cooperation with the TUD. The continuous photoneutron source utilises a tungsten radiator (Tungsten Photoneutron Source) to produce neutrons with a wide energy spectra. The TPNS uses the ELBE-accelerator as a source of electrons for neutron production. This process involves an intermediate step, where slowed down electrons produce bremsstrahlung (γ -rays) absorbed by tungsten nuclei. Consecutively, the excited nuclei emit neutrons. The neutron flux of the photoneutron source is five orders of magnitude higher than the flux of the DT neutron sources with appropriate moderation. The neutron spectrum of TPNS can be modified by moderators, in such a way that the spectrum is comparable to that in the first wall of a Tokamak-Reactor. That allows investigations with the typical neutron spectrum of the fusion reactor. The technical solution, initial operation and the first experiment are described in this work. The neutron source is, in particular, dedicated to quantitative investigations in fusion neutronics. A fusion reactor produces radioactive isotopes as a nuclear waste. The main activity is accumulated in the structural materials. Carefully selected structural materials can significantly minimize the activity and thereby the amount of nuclear waste. The purpose of this project is to find constructional materials with half-lives shorter than several years, which can be recycled after about 100 years. The work is divided into three parts. The first part is dedicated to the energy supply problem and nuclear fusion is addressed as a promising solution of the near future. The neutron laboratory housing the TPNS is also briefly described. The second part deals with the tungsten photoneutron source, the design, construction, operation and the first experiments for neutron production. The third part summarises results and presents an outlook for future experiments with the TPNS.

Das Institut für Kern- und Teilchenphysik (IKTP) der Technischen Universität Dresden (TUD) hat im Forschungszentrum Dresden-Rossendorf (FZD) ein Labor zur Untersuchung von neutroneninduzierten kernphysikalischen Prozessen in Materialien, die für die Fusionsforschung relevant sind, aufgebaut. Das Labor ist ausgestattet mit drei intensiven Neutronenquellen: einer 14 MeV-Neutronenquelle, einer weißen kontinuierlichen Photoneutronen-Quelle, die näher in dieser Arbeit beschrieben wird, und einer gepulsten Photoneutronen-Quelle, die vom FZD inKooperation mit der TUD aufgebaut wurde. Die kontinuierliche Photoneutronen-Quelle basiert auf einem Radiator aus Wolfram (engl. Tungsten Photoneutron Source (TPNS)). TPNS nutzt die im ELBE-Beschleuniger (Elektronen Linearbeschleuniger für Strahlen hoher Brillianz und niedriger Emittanz (ELBE)) beschleunigten Elektronen zur Neutronenerzeugung. Der Prozess läuft über Zwischenschritte ab, indem bei der Abbremsung der Elektronen im Radiator Bremsstrahlungsphotonen entstehen, die anschließend Neutronen durch (γ,xn)-Reaktionen erzeugen. Das Neutronenspektrum der TPNS kann mittels Moderatoren so modifiziert werden, dass es dem in der ersten Wand im Fusionsreaktor entspricht. Dies ermöglicht Untersuchungen mit einem für einen Fusionsreaktor typischen Neutronenspektrum. Die technische Verwirklichung des Projektes, die Inbetriebnahme der Anlage sowie die Durchführung der ersten Experimente zur Neutronenerzeugung ist Inhalt dieser Arbeit. Die Neutronenquelle ist insbesondere für qualitative Untersuchungen in der Fusionsneutronik bestimmt. Der Fusionsreaktor produziert, im Vergleich zu einem Spaltungsreaktor, keine langlebigen Isotope als Abfall. Die wesentliche Aktivität des Reaktors ist in Konstruktionsmaterialien akkumuliert. Durch sorgfältige Auswahl der Materialien kann man die Aktivierung minimieren und damit künftig wesentlich weniger radioaktives Inventar produzieren als in Spaltreaktoren. Ziel der kernphysikalischen Untersuchungen ist, solche Materialien für den Aufbau eines Fusionsreaktors zu erforschen, die niedrigaktivierbar sind, das heißt wenig Aktivität akkumulieren können, und eine Halbwertzeit von einigen Jahren haben. Es ist das Ziel, alle Konstruktionsmaterialien nach 100 Jahren wiederverwenden zu können. Die Neutronenflussdichte einer Photoneutronenquelle ist einige Größenordnungen höher als die, die mittels eines DT-Neutronengenerators mit anschließender Moderation erreicht werden kann. Die gesamte Arbeit ist in drei Teile geteilt. Der erste Teil leitet in die Problematik der Energieversorgung ein und zeigt die Kernfusion als eine vielversprechende Energiequelle der naher Zukunft auf. Das Neutronenlabor der TUD, in dem die TPNS aufgebaut ist, wird ebenfalls kurz vorgestellt. Der zweite Teil befasst sich mit der TPNS selbst, mit ihrem physikalischen Entwurf, der Konstruktion und dem Aufbau bis zu der Inbetriebnahme sowie dem ersten Experiment an der TPNS. Der letzte, dritte Teil ist die Zusammenfassung der vorhandenen Ergebnisse und gibt einen Ausblick auf die zukünftige Vorhaben. / The Institute for Nuclear and Particle Physics at the Technische Universität Dresden (TUD) has build a neutron physics laboratory at Forschungszentrum Dresden-Rossendorf (FZD) to investigate nuclear processes in materials. The experiments are focused on materials relevant to nuclear fusion. The laboratory is equipped with three intensive neutron sources. The first is a 14 MeV monochromatic neutron source based on the DT reaction (owned by TUD); the other two are continuous and pulsed white photoneutron sources based on (γ,xn) reactions. One pulsed photoneutron source is realized by FZD in cooperation with the TUD. The continuous photoneutron source utilises a tungsten radiator (Tungsten Photoneutron Source) to produce neutrons with a wide energy spectra. The TPNS uses the ELBE-accelerator as a source of electrons for neutron production. This process involves an intermediate step, where slowed down electrons produce bremsstrahlung (γ -rays) absorbed by tungsten nuclei. Consecutively, the excited nuclei emit neutrons. The neutron flux of the photoneutron source is five orders of magnitude higher than the flux of the DT neutron sources with appropriate moderation. The neutron spectrum of TPNS can be modified by moderators, in such a way that the spectrum is comparable to that in the first wall of a Tokamak-Reactor. That allows investigations with the typical neutron spectrum of the fusion reactor. The technical solution, initial operation and the first experiment are described in this work. The neutron source is, in particular, dedicated to quantitative investigations in fusion neutronics. A fusion reactor produces radioactive isotopes as a nuclear waste. The main activity is accumulated in the structural materials. Carefully selected structural materials can significantly minimize the activity and thereby the amount of nuclear waste. The purpose of this project is to find constructional materials with half-lives shorter than several years, which can be recycled after about 100 years. The work is divided into three parts. The first part is dedicated to the energy supply problem and nuclear fusion is addressed as a promising solution of the near future. The neutron laboratory housing the TPNS is also briefly described. The second part deals with the tungsten photoneutron source, the design, construction, operation and the first experiments for neutron production. The third part summarises results and presents an outlook for future experiments with the TPNS.