[en] A new accelerator, designated Proto-II, is presently under construction at Sandia Laboratories. Proto-II will have a nominal output of 100 kJ into a two-sided diode at a voltage of 1.5 MV and a total current of over 6 MA for 24 ns. This accelerator will be utilized for electron beam fusion experiments and for pulsed power and developmental studies leading to a proposed further factor of five scale-up in power. The design of Proto-II is based upon recent water switching developments and represents a 10-fold extrapolation of those results. Initial testing of Proto-II is scheduled to begin in 1976. Proto-II power flow starts with eight Marx generators which charge 16 water-insulated storage capacitors. Eight triggered, 3 MV, SF₆ gas-insulated switches next transfer the energy through oil-water interfaces into the first stage of 16 parallel lines. Next, the 16 first stages transfer their energy into the pulse forming lines and fast switching sections.The energy is then delivered to two converging, back-to-back, disk-shaped transmission line. Two back-to-back diodes then form the electron beams which are focused onto a common anode

[en] A new accelerator, designated Proto-II, presently under construction, will have a nominal output of 100 kJ into a two-sided diode at a voltage of 1.5 MV and a total current of over 6 MA for 24 ns. This accelerator will be utilized for electron beam fusion experiments and for pulsed power and developmental studies leading to a proposed further factor of five scale-up in power. The design of Proto-II is based upon recent water switching developments and represents a 10-fold extrapolation of those results. Initial testing of Proto-II is scheduled to begin in 1976. Proto-II power flow starts with eight Marx generators which charge 16 water-insulated storage capacitors. Eight triggered, 3 MV, SF₆ gas-insulated switches next transfer the energy through oil-water interfaces into the first stage of 16 parallel lines. Next, the 16 first stages transfer their energy into the pulse forming lines and fast switching sections. The energy is then delivered to two converging, back-to-back, disk-shaped transmission lines. Two back-to-back diodes then form the electron beams which are focused onto a common anode

[en] Genes in the recombinational repair pathway in the yeast Saccharomyces cerevisiae confer resistance to x-ray irradiation. Mutations in these genes disrupt the repair of double-stranded DNA breaks with multiple phenotypic effects such as abnormalities in meiosis and recombination. This epistasis group includes the genes RAD50 to RAD57. As discussed in previous annual reports, we have cloned many of these genes and are using the clones for molecular analyses of these genes. During the past year we have continued these studies, with particular emphasis on the transcriptional regulation of RAD51, RAD52 and RAD54, and the sequencing of RAD51. In addition we have initiated molecular research on RAD24, a gene involved in several DNA repair pathways in yeast. 7 refs., 1 fig

[en] In this work we present a keV-scale sterile-neutrino search with a low-tritium-activity data set of the KATRIN experiment, acquired in a commissioning run in 2018. KATRIN performs a spectroscopic measurement of the tritium β-decay spectrum with the main goal of directly determining the effective electron anti-neutrino mass. During this commissioning phase a lower tritium activity facilitated the measurement of a wider part of the tritium spectrum and thus the search for sterile neutrinos with a mass of up to 1.6 keV. We do not find a signal and set an exclusion limit on the sterile-to-active mixing amplitude of sin${}^2$θ < 5 × 10${}^{-<!--\; ???\; -->4}$ (95% C.L.) at a mass of 0.3 keV. This result improves current laboratory-based bounds in the sterile-neutrino mass range between 0.1 and 1.0 keV.

[en] The two major barriers to successful allogeneic bone marrow transplantation (BMT) in animals and man are graft-vs.-host disease (GVHD) and the risk of graft rejection. GVHD is the result of alloreactivity of mature donor T-lymphocytes present in the graft-vs.-host tissues and can be completely prevented by pregraft depletion of T-lymphocytes. Graft rejection results from residual host immunocompetent lymphocytes that survive heavy chemoradiotherapy prior to allogeneic BMT. Host resistance to allograft cannot be eradicated even by conventional conditioning with high-dose cyclophosphamide (120 mg/kg) and lethal whole body irradiation (1,200 rad). In the present report we have utilized two new techniques to overcome GVHD and graft rejection following allogeneic BMT. GVHD can be prevented by a new monoclonal rat antihuman lymphocyte antibody, CAMPATH-1, which binds human complement, enabling donor serum to serve as the source of complement. Prevention of rejection of T-lymphocyte-depleted marrow allografts can be achieved by the application of total lymphoid irradiation (TLI) in addition to conventional chemoradiotherapy, prior to allogeneic BMT. TLI causes potent immunosuppression with minimal side effects. A combination of TLI for overcoming host resistance to allograft, and CAMPATH-1 for overcoming GVHD, leads to a relatively smooth posttransplant outcome with no evidence of GVHD and with no need for posttransplant immunosuppression

[en] The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to determine the effective electron (anti)-neutrino mass with a sensitivity of 0.2eV/c${}^2$ by precisely measuring the endpoint region of the tritium β-decay spectrum. It uses a tandem of electrostatic spectrometers working as magnetic adiabatic collimation combined with an electrostatic (MAC-E) filters. In the space between the pre-spectrometer and the main spectrometer, creating a Penning trap is unavoidable when the superconducting magnet between the two spectrometers, biased at their respective nominal potentials, is energized. The electrons accumulated in this trap can lead to discharges, which create additional background electrons and endanger the spectrometer and detector section downstream. To counteract this problem, “electron catchers” were installed in the beamline inside the magnet bore between the two spectrometers. These catchers can be moved across the magnetic-flux tube and intercept on a sub-ms time scale the stored electrons along their magnetron motion paths. In this paper, we report on the design and the successful commissioning of the electron catchers and present results on their efficiency in reducing the experimental background.

[en] The KATRIN experiment is designed for a direct and model-independent determination of the effective electron anti-neutrino mass via a high-precision measurement of the tritium β-decay endpoint region with a sensitivity on m${}_{\mathrm{\nu <!--\; ??\; -->}}$ of 0.2 eV/c${}^2$ (90% CL). For this purpose, the β-electrons from a high-luminosity windowless gaseous tritium source traversing an electrostatic retarding spectrometer are counted to obtain an integral spectrum around the endpoint energy of 18.6 keV. A dominant systematic effect of the response of the experimental setup is the energy loss of β-electrons from elastic and inelastic scattering off tritium molecules within the source. We determined the energy-loss function in-situ with a pulsed angular-selective and monoenergetic photoelectron source at various tritium-source densities. The data was recorded in integral and differential modes; the latter was achieved by using a novel time-of-flight technique. We developed a semi-empirical parametrization for the energy-loss function for the scattering of 18.6-keV electrons from hydrogen isotopologs. This model was fit to measurement data with a 95% T${}_2$ gas mixture at 30 K, as used in the first KATRIN neutrino-mass analyses, as well as a D${}_2$ gas mixture of 96% purity used in KATRIN commissioning runs. The achieved precision on the energy-loss function has abated the corresponding uncertainty of σ(m${}_{\mathrm{\nu <!--\; ??\; -->}}^2$) <10${}^{-<!--\; ???\; -->2}$eV${}^2$ in the KATRIN neutrino-mass measurement to a subdominant level.

[en] The KArlsruhe TRItium Neutrino (KATRIN) experiment, which aims to make a direct and model-independent determination of the absolute neutrino mass scale, is a complex experiment with many components. More than 15 years ago, we published a technical design report (TDR) [1] to describe the hardware design and requirements to achieve our sensitivity goal of 0.2 eV at 90% C.L. on the neutrino mass. Since then there has been considerable progress, culminating in the publication of first neutrino mass results with the entire beamline operating [2]. In this paper, we document the current state of all completed beamline components (as of the first neutrino mass measurement campaign), demonstrate our ability to reliably and stably control them over long times, and present details on their respective commissioning campaigns. (technical report)