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The results of the preparation of strengthened syntactic carbon materials that can be used for industrial-grade heat insulation in conditions of heightened pressures and temperatures are presented. Strengthened syntactic carbon material is obtained by mixing hollow carbon microspheres, pre-treated with vanadium (III) chloride catalyst, with a phenol-formaldehyde binder with the addition of fine polydimethylsilane, molding the composition at low pressure, soaking the mold at 150°C for 2 h, followed by heat treatment in an inert environment at 375°C and final carbonization in combination with carbidization when the temperature rises at a rate of 100 K/h to 900°C. The physicomechanical and thermophysical characteristics were studied. Syntactic material can be used for the manufacture of heat-insulation products operating at high temperatures.

Abstract—Exposure of cultured neurons to high concentrations of Glu leads to a strong depolarization of mitochondria, which develops synchronously with the secondary rise in the intracellular Ca2+ concentration (delayed calcium deregulation, DCD). In this study, using the primary culture of rat cerebellar neurons, we investigated the mechanism of neuronal sensitization, which manifests itself in the reduction of latent periods of DCD during repeated exposures to Glu. It was shown that the most likely cause of sensitization is the inability of mitochondria to maintain a high transmembrane potential (ΔΨm) as a result of an increase in the proton conductivity of the internal mitochondrial membrane, but not the opening of the mitochondrial permeability transition pore in the inner mitochondrial membrane. Mitochondrial dysfunction reduces the production of ATP, leading to the inability of neurons to quickly restore the concentration of Na+, ATP, and NADH in the intervals between successive Glu administrations. One of the reasons that aggravate the dysfunction of mitochondria and contribute to the sensitization of neurons to the repeated action of Glu is Ca2+ accumulated in the mitochondria during the first glutamate impact.

We studied the effects of selective inhibitors of neuronal and inducible NO-synthase (7-nitroindazole and aminoguanidine) and non-selective NO-synthase inhibitor L-NAME on ATP content and survival of cultured rat cerebellar neurons during hyperstimulation of glutamate receptors with toxic doses of glutamate. Application of 100 μM glutamate reduced ATP content in the primary culture of 7-8- and 14-15-day-old cerebellar granule cells by 66 and 49%, respectively, in comparison with the control. Inhibition of nitric oxide synthesis with 7-nitroindazole during glutamate exposure in the culture of 7-8-day-old neurons and with 7-nitroindazole and aminoguanidine in the culture of 14-15-day-old neurons ensured better protection of cells from ATP level decrease than non-specific inhibition with L-NAME. In addition, inhibition of neuronal and inducible NO-synthase during glutamate exposure decreased death of “young” neurons, whereas death of “old” neurons remained high under these conditions.

The MTT assay based on the reduction of 3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium in the cell cytoplasm to a strongly light absorbing formazan is among the most commonly used methods for determination of cell viability and activity of NAD-dependent oxidoreductases. In the present study, the effects of MTT (0.1 mg/ml) on mitochondrial potential (ΔΨ m ), intracellular NADH, and respiration of cultured rat cerebellum neurons and isolated rat liver mitochondria were investigated. MTT caused rapid quenching of NADH autofluorescence, fluorescence of MitoTracker Green (MTG) and ΔΨ m -sensitive probes Rh123 (rhodamine 123) and TMRM (tetramethylrhodamine methyl ester). The Rh123 signal, unlike that of NADH, MTG, and TMRM, increased in the nucleoplasm after 5-10 min, and this was accompanied by the formation of opaque aggregates of formazan in the cytoplasm and neurites. Increase in the Rh123 signal indicated diffusion of the probe from mitochondria to cytosol and nucleus due to ΔΨ m decrease. Inhibition of complex I of the respiratory chain decreased the rate of formazan formation, while inhibition of complex IV increased it. Inhibition of complex III and ATP-synthase affected only insignificantly the rate of formazan formation. Inhibition of glycolysis by 2-deoxy-D-glucose blocked the MTT reduction, whereas pyruvate increased the rate of formazan formation in a concentration-dependent manner. MTT reduced the rate of oxygen consumption by cultured neurons to the value observed when respiratory chain complexes I and III were simultaneously blocked, and it suppressed respiration of isolated mitochondria if substrates oxidized by NAD-dependent dehydrogenases were used. These results demonstrate that formazan formation in cultured rat cerebellum neurons occurs primarily in mitochondria. The initial rate of formazan formation may serve as an indicator of complex I activity and pyruvate transport rate.

A bstract Heavy Neutral Leptons (HNLs) are hypothetical particles predicted by many extensions of the Standard Model. These particles can, among other things, explain the origin of neutrino masses, generate the observed matter-antimatter asymmetry in the Universe and provide a dark matter candidate. The SHiP experiment will be able to search for HNLs produced in decays of heavy mesons and travelling distances ranging between O (50 m) and tens of kilometers before decaying. We present the sensitivity of the SHiP experiment to a number of HNL’s benchmark models and provide a way to calculate the SHiP’s sensitivity to HNLs for arbitrary patterns of flavour mixings. The corresponding tools and data files are also made publicly available.

The Search for Hidden Particles (SHiP) Collaboration has proposed a general-purpose experimental facility operating in beam-dump mode at the CERN SPS accelerator to search for light, feebly interacting particles. In the baseline configuration, the SHiP experiment incorporates two complementary detectors. The upstream detector is designed for recoil signatures of light dark matter (LDM) scattering and for neutrino physics, in particular with tau neutrinos. It consists of a spectrometer magnet housing a layered detector system with high-density LDM/neutrino target plates, emulsion-film technology and electronic high-precision tracking. The total detector target mass amounts to about eight tonnes. The downstream detector system aims at measuring visible decays of feebly interacting particles to both fully reconstructed final states and to partially reconstructed final states with neutrinos, in a nearly background-free environment. The detector consists of a 50m long decay volume under vacuum followed by a spectrometer and particle identification system with a rectangular acceptance of 5 m in width and 10 m in height. Using the high-intensity beam of 400GeV protons, the experiment aims at profiting from the 4×1019 protons per year that are currently unexploited at the SPS, over a period of 5–10 years. This allows probing dark photons, dark scalars and pseudo-scalars, and heavy neutral leptons with GeV-scale masses in the direct searches at sensitivities that largely exceed those of existing and projected experiments. The sensitivity to light dark matter through scattering reaches well below the dark matter relic density limits in the range from a few MeV/c2 up to 100 MeV-scale masses, and it will be possible to study tau neutrino interactions with unprecedented statistics. This paper describes the SHiP experiment baseline setup and the detector systems, together with performance results from prototypes in test beams, as it was prepared for the 2020 Update of the European Strategy for Particle Physics. The expected detector performance from simulation is summarised at the end.

Dark photons are hypothetical massive vector particles that could mix with ordinary photons. The simplest theoretical model is fully characterised by only two parameters: the mass of the dark photon mγD and its mixing parameter with the photon, ε. The sensitivity of the SHiP detector is reviewed for dark photons in the mass range between 0.002 and 10 GeV. Different production mechanisms are simulated, with the dark photons decaying to pairs of visible fermions, including both leptons and quarks. Exclusion contours are presented and compared with those of past experiments. The SHiP detector is expected to have a unique sensitivity for mγD ranging between 0.8 and 3.3-0.5+0.2 GeV, and ε2 ranging between 10-11 and 10-17.

A bstract Dark matter is a well-established theoretical addition to the Standard Model supported by many observations in modern astrophysics and cosmology. In this context, the existence of weakly interacting massive particles represents an appealing solution to the observed thermal relic in the Universe. Indeed, a large experimental campaign is ongoing for the detection of such particles in the sub-GeV mass range. Adopting the benchmark scenario for light dark matter particles produced in the decay of a dark photon, with α D = 0 . 1 and m A ′ = 3 m χ , we study the potential of the SHiP experiment to detect such elusive particles through its Scattering and Neutrino detector (SND). In its 5-years run, corresponding to 2 · 10 20 protons on target from the CERN SPS, we find that SHiP will improve the current limits in the mass range for the dark matter from about 1 MeV to 300 MeV. In particular, we show that SHiP will probe the thermal target for Majorana candidates in most of this mass window and even reach the Pseudo-Dirac thermal relic.

The work examines the mechanism of central nerve cell death upon stimulation of brain NMDA receptors with the stimulatory mediator glutamate. A prolonged stimulation of neurons with glutamate is known to result in the disorder of Ca 2+ homeostasis and severe mitochondrial depolarization followed by cell death. It has been shown that the overload of mitochondria with Sr 2+ leads to the release of the cation, medium alkalization, decrease of membrane potential and mitochondrial swelling, indicating a nonspecific permeabilization of the mitochondrial membrane. The permeabilization, in our opinion, is caused by the activation of Ca 2+ /Sr 2+ -dependent phospholipase A 2 (PLA 2 ), resulting in the formation of free palmitic and stearic acids in the mitochondrial membrane. These fatty acids bind Ca 2+ with high affinity and the process of binding is accompanied by the formation of a transient lipid pore—a phenomenon demonstrated earlier on both artificial and mitochondrial membranes. The inhibitors of PLA 2 have been shown to suppress permeabilization of mitochondrial membranes. In the culture of granular cerebellum neurons, the PLA 2 inhibitors prolonged the lag of the delayed Sr 2+ deregulation and membrane depolarization. On the basis of data obtained on isolated mitochondria and neurons we suppose that the initial stages of glutamate-induced Ca 2+ deregulation of neurons are underlain by the opening of lipid pores in brain mitochondria.

The SHiP experiment is proposed to search for very weakly interacting particles beyond the Standard Model which are produced in a 400 GeV/c proton beam dump at the CERN SPS. About 10 11 muons per spill will be produced in the dump. To design the experiment such that the muon-induced background is minimized, a precise knowledge of the muon spectrum is required. To validate the muon flux generated by our Pythia and GEANT4 based Monte Carlo simulation (FairShip), we have measured the muon flux emanating from a SHiP-like target at the SPS. This target, consisting of 13 interaction lengths of slabs of molybdenum and tungsten, followed by a 2.4 m iron hadron absorber was placed in the H4 400 GeV/c proton beam line. To identify muons and to measure the momentum spectrum, a spectrometer instrumented with drift tubes and a muon tagger were used. During a 3-week period a dataset for analysis corresponding to ( 3.27 ± 0.07 ) × 10 11 protons on target was recorded. This amounts to approximatively 1% of a SHiP spill.