Stimulation of the Growth of Juvenile North African Catfish Clarias gariepinus by Modification of the Water Oxidation–Reduction Potential

Biology Bulletin - The effect of water with a high negative oxidation–reduction potential (ORP) on the physiological parameters of juvenile North African catfish (Clarias gariepinus) has been...     

Hexuronates influence the oligomeric form of the Dps structural protein of bacterial nucleoid and its ability to bind to linear DNA fragments

Proteins of the Dps family perform a dual function in bacterial cells. As ferritins, they protect cells from destructive effects of Fe²⁺ ions, while interacting with DNA they condense the genome in the absence of nutrients. The ability of Dps to self-aggregate is of a great importance. The way of genome remodelling from the condensed state to the active one is not yet known. Here, the effects of two sugar ligands on Dps interaction with DNA have been studied in vitro. For the first time it was demonstrated that D-glucuronate and D-galacturonate, but not D-glucose, can decompose the dodecameric structure of the protein and D-glucuronate stimulated the formation of binary complexes with the linear DNA fragments. As a result of flexible molecular docking, it was found that the molecules of all three sugars potentially can form clusters inside the protein cavity of Dps, but D-glucuronate and D-galacturonate were also bound in the region of intersubunit contacts of oligomer. The consequent destabilization of the intersubunit bonding network can, thus, be the main factor provoking the protein decay to the smaller oligomeric forms. Such a structural rearrangement, leading to a reduction in aggregation, may play a key role in genome decondensation during cell transition to the phase of rapid growth.     

Plasma relativistic microwave amplifier with smooth frequency tuning from 2.4 to 3.2 GHz

Earlier, it was shown that the plasma relativistic microwave amplifier can operate at two frequencies, 2 and 3.2 GHz. In the present work, it is shown that, by varying the plasma density from one microwave pulse to another, it is possible to amplify the input signals to a power of 50?C80 MW at any frequency in the range 2.4?C3.2 GHz.     

Noise characteristics of a plasma relativistic microwave amplifier

Reasons for the occurrence of microwave noise at the output of a plasma relativistic amplifier have been analyzed. It is found that, in the absence of an input signal, the emission spectrum of the plasma relativistic microwave amplifier is similar to that of an electron beam in vacuum. It is concluded that microwave noise at the output of the amplifier appears as a result of amplification of the intrinsic noise of the electron beam. The emission characteristics of a relativistic electron beam formed in a magnetically insulated diode with an explosive emission cathode in vacuum have been studied experimentally for the first time. An important point is that, in this case, there is no virtual cathode in the drift space.     

Ultrawideband Plasma Relativistic Microwave Source

Plasma Physics Reports - An ultrawideband (UWB) plasma relativistic microwave source based on the amplification of self-noise of a relativistic electron beam in plasma is described. There is a...     

Output power variations in a plasma relativistic microwave amplifier during a 500-ns relativistic electron beam current pulse

A relativistic plasma microwave amplifier with a gain of about 30 dB and an output power of about 60–100 MW in the frequency range from 2.4 to 3.2 GHz is studied experimentally. The total duration of the output microwave pulse is equal to the duration of the current pulse of the driving relativistic electron beam (500 ns); however, the maximum output power is observed only within 200 ns. It is shown that variations in the output microwave power during the current pulse of the annular relativistic electron beam are caused by variations in the beam radius and thickness. Analysis of the experimental data and results of numerical simulations show that the thickness of the electron beam is determined by the density of the cathode emission current.     

Structural rearrangements of the cerebral cortex in children and adolescents

The cortical formations of the brain involved in visual functions (the occipital and temporo-parieto- occipital areas, the oculomotor area of the prefrontal cortex), as well as the motor cortex in the representation zone of the arm and the medial region of the frontal cortex adjacent to the limbic lobe, were studied in post-mortem material. The thickness of the cortex and cortical layer III, the sizes of pyramidal neurons, the specific volumes of neurons and intracortical vessels were studied in subjects of both sexes, from birth to the age of 20 years, at yearly intervals (103 observations) using histological techniques, computer morphometric and stereological analysis. The thickness of the cortex of the cerebral hemispheres was observed to intensively increase from birth to the age of 3 years in the occipital, temporo-parieto-occipital and prefrontal cortical areas involved in visual recognition processes. The increase in thickness of the cerebral cortex continues until the age of 6 in the occipital cortex and in the oculomotor area, until the age of 7 years in the temporo-parietooccipital area and the medial prefrontal area, and until the age of 8–9 years in the motor cortex. The sizes of pyramidal neurons increase until the age of 6 years in the motor cortex, until the age of 8 years on the medial surface of the frontal lobe, and until the age of 9–10 years in the temporo-parieto-occipital area and in the dorsolateral area of the prefrontal cortex. The specific volume of neurons and blood vessels in the cortex of the cerebral hemispheres decreases and the volume of intracortical fibers increases throughout the ascending ontogeny, which is manifested most intensively in the prefrontal cortex.     

Spectra of Plasma Relativistic Microwave Amplifier of Monochromatic Signal

Plasma Physics Reports - The ratio of the radiation energy of the plasma relativistic microwave amplifier at a frequency of the input signal to the noise energy is measured. In the absence of the...