DOI: 10.7256/2453-8884.2018.4.28130

Abstract: Due to the low power consumption, CMOS structures are preferred for creating large and ultra-large integrated circuits. However, the reliability of the circuits is largely limited by the latch phenomenon that occurs in CMOS structures. The electrical characteristic of the latch up phenomenon in a CMOS integrated circuit is characterized by the presence of a number of anomalous phenomena. These effects distort and make ambiguous the results of measuring the electrical sensitivity of the circuits to the latch. The development of microelectronics is constantly striving to reduce the size of the elements of integrated circuits, in particular transistors. Reducing the size of integrated circuits leads to the amplification of short-channel effects in MOS transistors. When reducing the size of integral elements, various options for scaling devices with a metal-oxide-semiconductor structure are considered. The mechanisms that cause the appearance of the snap-in do not depend on the conductivity type of the semiconductor region of the pocket.

DOI: 10.7256/2453-8884.2018.4.28448

Abstract: The greatest success of ion implantation has been achieved in the field of planar technology of semiconductor devices and integrated circuits. The development of devices with elements of nanoparticles, including the active region of which are metal nanoparticles in a dielectric matrix, has been greatly developed. The aim of the work is to simulate the process of ion implantation of a structure consisting of gold nanoparticles in a silicon dioxide matrix and calculations of the distribution of doping ions, cascades of displaced matrix ions and nanoparticles, as well as the distribution of ions reflected from the nanoparticles. The implantation conditions vary depending on the position of the projection of a point on the surface of the structure on the horizontal radius of the nanoparticle from the center to the periphery. A physical model of the process of ion implantation of gold nanoparticles located in a silicon dioxide matrix has been compiled. The process of ionic doping of the structure with boron and arsenic ions was simulated for different cross sections, and graphs of the distribution of doping ions, recoil atoms, reflected and sputtered ions were obtained depending on the coordinate from the center of the nanoparticle.

DOI: 10.7256/2453-8884.2018.3.27423

Abstract: The processes of formation of radiation-resistant heterostructures with required set of structural and electrophysical parameters, taking into account the influence of ionizing radiation effects, allowing to expand the field of their application and improve the reliability of electronic equipment are described. The influence of irradiation on the parameters of hetero- and semiconductor structures made according to various design-technological variants is studied. It is shown that the charge density in the dielectric increases with increasing dose of ionizing particles, reaches saturation at a dose of 108- 109 rad, and the value of the built-in charge and mechanical stresses in multilayer dielectric systems decrease due to the formation of an intermediate charge at the dielectric interface and the presence of a potential barrier between them. By adjusting the rate of introduction and characteristics of radiation centers during irradiation type, method of growing and the level of doping material, and the integrated flux density of the irradiation, the sample temperature during irradiation may purposefully alter the electrical properties of heterostructures and electrical parameters of devices and integrated circuits. Developed methods, for radiation resistant heterostructures forming, reduces charge formation at silicon-oxide interface. SOI technology on optimized structure, shows good results, even at high radiation doses. The resistance to the total dose of radiation rises by three orders of magnitude.

DOI: 10.7256/2453-8884.2017.4.24868

Abstract: Aluminum and its alloys are the main metallization materials. With an increase in degree of integration the role of interconnections rises: they occupy a growing area of the crystal, the density of the package increases, which leads to a decrease in the thickness and width of the conductive tracks. In nanodimensional structures the value of the current density sufficient for the development of electromigration effects occurs at currents of 50-100 mA. The article explores the factors affecting the mechanism of destruction of the integrated circuits' metallization due to electromigration. The author studies metallization lines at different stages of their destruction by electromigration with the help of raster scanning and transmission electron microscopes. In general, the main problem associated with high-temperature application of aluminum metallization is the large grain size and surface roughness, which makes alignment on such a metal layer difficult. The results of the experiments lead to the conclusion that geometric factors play a dominant role in the mechanism of destruction of metallization of integrated circuits due to electromigration.

DOI: 10.7256/2453-8884.2017.3.23345

Abstract: Aluminium with its alloys is the basic material of integrated circuits metallization. Use of VLSIC toughens the requirements to the parameters of metallization, which determine its reliability, such as surface resistance, step coating quality, number and sizes of tension-caused voids, and electromigration tolerance. Poor quality of metallization is one of the most dangerous defects in semiconductor technology of integrated circuits. Electromigration can cause failure when passing high-density current through metallization. The materials have been tested in order to estimate the intensity of metal resistance variation caused by electromigration. Based on the results of these tests, the authors conclude that geometrical factors play a dominant role in the mechanism of erosion of integrated circuits metallization caused by electromigration. With regard to the tests, the authors formulate recommendations about the transition from the sputtering technique to evaporation deposition.