{"title":"Obtaining of aluminum nano-powders by thermal treatment","authors":"G. Paskalov, Usa Plasma Microsystems Llc","doi":"10.26577/phst-2019-1-p8","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p8","url":null,"abstract":"It is known that the formation of a dispersed phase under extreme conditions (high temperatures andprocess speed) leads to the formation of a non-equilibrium structure of particles. Therefore, the first toattract attention are technologies based on pulsed processes with high rates of change in the thermodynamicparameters of the system. One of these promising methods for obtaining a wide range of nano-powders ofinorganic materials is the technology based on the process of electrical explosion of a conductor (EVP, EVPtechnology) [1-5]. Unfortunately, this method is not applicable on industrial scales. In this thesis, productionof Al nanoparticles by hydrogen reduction of metal chlorides in gas phase was studied. Nanoparticles haveunique properties not found in bulk or micron-scale materials. These enable new products or reduced useof raw materials. Metal nanoparticle production has been studied widely, but especially for coated metalparticles, research of coating mechanisms and economic production methods is still needed. The usedmethod combines a high yield, a high production rate, low production costs, high particle quality, and agood range of available particle number average diameters and other properties. Control of the productparameters has been carried out by using a special quenching system and plasma reactor configuration.Highly hydrogen enriched Al nanopowder were collected in metal form and tested for different applications.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"9 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"131577776","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
D. Schur, A. Zolotarenko, A. Zolotarenko, E. P. Zolotarenko, M. V. Chimbai, A. Zolotarenko, N. Akhanova, M. Sultangazina
{"title":"Analysis and identification of platinum-containing nanoproducts of plasma-chemical synthesis in a gaseous medium","authors":"D. Schur, A. Zolotarenko, A. Zolotarenko, E. P. Zolotarenko, M. V. Chimbai, A. Zolotarenko, N. Akhanova, M. Sultangazina","doi":"10.26577/phst-2019-1-p9","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p9","url":null,"abstract":"This article studies a nanoproduct that is formed by simultaneous plasma-chemical evaporation ofgraphite and platinum. It was shown that the resulting deposits under different synthesis conditions havea similar and well-defined structure and consist of two main parts (core and enclosing bark). The structureof both parts is investigated at the micro- and nanoscale levels. The products of synthesis and similarproducts obtained without the use of platinum has been compared. The distribution of platinum in synthesisproducts is studied. It is proved that the atoms of the platinum catalyst influence the process of formationof the deposit. Namely, it stimulates the formation of a deposit where the deposit core containing platinumcontainingbundles of CNT exists as an independent core that does not have a strong connection with thedeposit shell. It is found that differential-thermal analysis of CNM in air by the methods of TG, DTG, DTAallows to reveal insignificant differences in the heat resistance of different carbon nanostructures, and thusit can be used for their identification. Such studies are of great importance for the synthesis of platinumcontainingcatalysts for fuel cells and other chemical industries.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"73 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"114564774","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"The fundamental equation of the field theory in De Sitter pulse space","authors":"R. Ibadov, S. Murodov","doi":"10.26577/PHST-2019-1-P4","DOIUrl":"https://doi.org/10.26577/PHST-2019-1-P4","url":null,"abstract":"The fundamental equation of the field theory in De Sitter pulse 5-dimensional space is obtained. Thewave function, subordinated to this equation in usual space-time, doubles. One of these functions,probably to consider as the candidate on “the Phantom field” responsible for expansion of the Universewith acceleration. Some experimental consequences are predicted. In all these calculations thepolarization of particles be taken into account. The Lagrangian of quantum electrodynamics with thefundamental mass is chosen as an effective interaction Lagrangian. All the calculations are made in theEuclidian space, the transfer to the ordinary pseudoeuclidian space is established in the final expressionsonly. The approach has been based on the assumption that the momentum space possesses the geometricstructure of a de Sitters pace of constant curvature. A key role has been be assigned to this constant radiusof curvature.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"21 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"130885894","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Asymptotic behavior of numerical solutions of the Schrodinger equation","authors":"F. Pen'kov, P. Krassovitskiy","doi":"10.26577/phst-2019-1-p3","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p3","url":null,"abstract":"Many problems of numerically solving the Schrodinger equation require that we choose asymptoticdistances many times greater than the characteristic size of the region of interaction. The problems ofresonance diffraction for composite particles or the problem of nucleon scattering by nonspherical atomicnuclei are examples of the need to use a large spatial domain for calculations. If the solution to onedimensionalequations can be immediately chosen in a form that preserves unitarity, the invariance ofprobability (in the form of, e.g., fulfilling an optical theorem) is a real problem for two-dimensionalequations. An addition that does not exceed the discretization error and ensures a high degree of unitarityis proposed as a result of studying the properties of a discrete two-dimensional equation.The problem for scattering of rigid molecules by the disks was successfully solved using an improvedsampling scheme that provides the correct asymptotic behavior. Corresponding diffraction scatteringcurves are of a pronounced resonance nature.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"59 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"130774159","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"The first excited 1/2+ state in 9Be and 9B","authors":"M. Odsuren, Y. Kikuchi, T. Myo, K. Katō","doi":"10.26577/phst-2019-1-p7","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p7","url":null,"abstract":"Nuclear states observed around threshold energies provide us with interesting problems associated withthe nuclear cluster structure [1, 2, 3, 4]. The first excited Jπ = 1/2+ state of 9Be [5], which is an α+ α + nBorromean nucleus, is one of the typical examples in light nuclei. This state of 9Be has been observed as asharp peak above the 8Be + n threshold energy in the photo-disintegration cross section of γ+9Be→ α + α+ n [6, 7]. The strength of the peak has a strong influence on the reaction rate of the 9Be synthesis. Weperformed the calculations using an α + α + n three-body model [8, 9] and the complex scaling method(CSM), which well reproduces the observed photo-disintegration cross section. However, the resultindicates that the 1/2+ state shows the s-wave virtual-state character of 8Be+n. In addition to this problem,we discuss a mirror state problem of the first excite 1/2+ state in 9B.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"1 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"130394204","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
K. Mukashev, A.Kh. Arginova, A. D. Baisenova, Bakhtiyar Iskakov, R. Mukhamedshin, O. Novolodskaya, V. Piskal, V. Ryabov, T. Sadykov, A. Serikkanov, Y. M. Tautaev, V. Zhukov, N. N. Zastrozhnova
{"title":"Search for structures in the distribution of particles from the central area of wide atmospheric showers conducted on the Adron-55 installation","authors":"K. Mukashev, A.Kh. Arginova, A. D. Baisenova, Bakhtiyar Iskakov, R. Mukhamedshin, O. Novolodskaya, V. Piskal, V. Ryabov, T. Sadykov, A. Serikkanov, Y. M. Tautaev, V. Zhukov, N. N. Zastrozhnova","doi":"10.26577/phst-2019-1-p10","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p10","url":null,"abstract":"The ionization calorimeter “Adron-55”, located at an altitude of 3340 meters above sea level, is partof the unified registration system for the shower installation of the Tian-Shan high-mountain station. The“Hadron-55” installation is a 2-tier ionization calorimeter consisting of a shower system, a gamma blockand a hadron block located under it with a vertical air gap of 2.2 meters. The calorimeter consists of 6layers of ionization chambers with 144 chambers in each layer and a spatial resolution of the WASstructure equal to 11 cm. The total area of the calorimeter is 55 square meters with an absorber thicknessof 1150 g / cm2. The calorimeter also contains helium counters for recording the neutron component. Thecentral shower calorimeter system contains 30 scintillation detectors with an area of 400 m2 and 8peripheral Sc-detectors at a distance of up to 100 m. The total area of the entire recording system is ~30000 m2. Over 4 years of operation, more than 120,000 events with energies above 1015 eV have beenrecorded. Currently, the processing and analysis of the data being obtained are performed.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"66 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128642008","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"The plasma parameters and neutron yield at device of \"Plasma focus\"","authors":"A. Zhukeshov, Z. Moldabekov, A. Ioffe","doi":"10.26577/phst-2019-1-p2","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p2","url":null,"abstract":"Present work presents calculations and experimental studies on the formation and dynamics of plasma onthe “plasma focus” set up. Physical conditions were determined and critical parameters were calculatedfor estimating the neutron yield for kilojoule and megajoule set ups. The results of plasma diagnostics andflow formation in the CPA-30 and PF-4 set ups are also shown. A comparison of calculated data andexperimental values is performed. The value of the neutron yield parameter is justified and the possiblecause of the appearance of saturation is indicated. The rationale for the development of further research inthe direction of creating conditions for thermonuclear fusion in installations of the plasma focus type isgiven. The neutron flux was observed on high-voltage gas discharges with a specific geometry of theelectrodes. The result of measuring the anisotropy of the neutron yield along the axial z and radial φdirections was equal to Yn(z)/Yn(φ)~ 2 ÷ 3, which contradicts the thermonuclear mechanism.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"8 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"126289381","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
V. Dyachkov, Y. Zaripova, A. Yushkov, A. Shakirov, M. Bigeldiyeva, K. S. Dyussebayeva, K. E. Abramov
{"title":"Periodic variations in time of atmospheric alpha and beta radioactive nanoparticles","authors":"V. Dyachkov, Y. Zaripova, A. Yushkov, A. Shakirov, M. Bigeldiyeva, K. S. Dyussebayeva, K. E. Abramov","doi":"10.26577/phst-2019-1-p6","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p6","url":null,"abstract":"Here we present time variations data of radon emanations in the surface layer of the atmosphere,measured from January 2016 to June 2018. By means of spectral analysis method, we have analyzed timevariations and showed the presence of existing natural variations, mechanisms of which were describedby the authors in previous works. Authors measured the activity of natural beta-active radionuclides ofradon’s daughter decay products (DDP) in the surface layer of the atmosphere. The measurements wereperformed with a beta-spectrometer “Progress” scintillation detector, which is located on the third floor ofthe Faculty of Physics and Technology at al-Farabi Kazakh National University (KazNU). Measurementsof beta spectra were carried out with an exposure of at least for 2000 seconds and during the day up to 10beta spectra were recorded. The built up time dependence of the integral values of the spectra shows thatseasonal variations of natural beta-active radionuclides are manifested on the background of diurnalfluctuations. Thus, 1 day, 4 day, 7 day, 16 day and 30 day variations were found.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"611 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116076023","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"On three-cluster disintegration of 9Be","authors":"V. Vasilevsky, K. Katō","doi":"10.26577/phst-2019-1-p5","DOIUrl":"https://doi.org/10.26577/phst-2019-1-p5","url":null,"abstract":"We study a process of the photodisintegration of some Borromean light nuclei into three clusters. Thisstudy is performed within a three-cluster microscopic model. In Reference [1] this model was applied toobtain parameters of resonance states in 9Be and 9B and to establish their nature. Main aim of the presentinvestigations is to describe the dipole transition probability from the ground state of 9Be to the states ofthree-cluster α+α+n continuum by using the same model. That model exploits the hypersphericalharmonics basis (HHB) and thus reduces many-channel Schrodinger equation to the algebraic matrix(AM) form. The dipole transitions from the ground 3/2- state to the 1/2+ states of three-cluster continuumwere studied in detail. The role of resonance states in three-cluster continuum to this process isinvestigated in detail. The dominant channels with the maximal dipole strength due to the couplingbetween the ground and scattering states are discovered","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"10 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2019-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"130743911","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
M. Abishev, N. Beissen, B. Karsimanov, I. Uspanov, M. Alimkulova
{"title":"Stationar spherical-symmetric configuration of dark matter","authors":"M. Abishev, N. Beissen, B. Karsimanov, I. Uspanov, M. Alimkulova","doi":"10.26577/phst.2020.v7.i1.10","DOIUrl":"https://doi.org/10.26577/phst.2020.v7.i1.10","url":null,"abstract":"The article is devoted to the consideration of a model problem, where mass flow of dark matter which take as only gravitational interacting spherical continuous medium without pressure and with radial opposite motion with equilibrium ascending and descending components, starting free fall from boundary of the sphere and passing through the center, stopping and fall back at the boundary of the spherical mass distribution, which give us stationary spherical-symmetric configuration of dark matter. The presence of an opposite motion makes the configuration we are considering stationary. Limited mass and dimensions of the dark matter distribution gives us possibility to modelling galaxy galo and dark stars. This configuration is considered in the classical gravity. As a result of the study, we obtained a singular density distribution in the center and in the shell of sphere and corresponding velocity field with singular center. The resulting profile can be used to construct arbitrary distributions, corresponding to the observed profiles.","PeriodicalId":321102,"journal":{"name":"Physical Sciences and Technology","volume":"115 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"127518452","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}