8 research outputs found
Magnetic Characteristics of Mn-Implanted GaN Nanorods Followed by Thermal Annealing
We have investigated the magnetic and optical properties of dislocation-free vertical GaN nanorods with diameters of 150 nm grown on (111) Si substrates by radio-frequency plasma-assisted molecular-beam epitaxy followed by Mn ion implantation and annealing. The GaN nanorods are fully relaxed and have a very good crystal quality characterized by extremely strong and narrow photoluminescence excitonic lines near 3.47 eV. For GaMnN nanorods, it can be concluded that the ferromagnetic property of GaMnN nanorod with a Curie temperature over 300 K is associated with the formation of Mn 4 Si 7 magnetic phase which results from the effects of magnetic and structural disorder introduced by a random incorporation and inhomogeneous distribution of Mn atoms in the porous layer between the nanorods that form precipitates in the Si substrate before or during the annealing step amongst the GaN nanorods
Specific heat study of Ga1-xMnxAs
Specific heat measurements were used to study the magnetic phase transition
in Ga1-xMnxAs. Two different types of Ga1-xMnxAs samples have been
investigated. The sample with a Mn concentration of 1.6% shows insulating
behavior, and the sample with a Mn concentration of 2.6% is metallic. The
temperature dependence of the specific heat for both samples reveals a
pronounced lambda-shaped peak near the Curie temperature, which indicates a
second-order phase transition in these samples. The critical behavior of the
specific heat for Ga1-xMnxAs samples is consistent with the mean-field behavior
with Gaussian fluctuations of the magnetization in the close vicinity of TC.Comment: 12 pages, 5 figure
Π Π°Π΄ΠΈΠΎΠΏΠΎΠ³Π»ΠΎΡΠ°ΡΡΠΈΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ»ΠΈΡΡΠΈΠ»Π΅Π½Π°
Π Π°Π΄ΠΈΠΎΠΏΠΎΠ³Π»ΠΎΡΠ°ΡΡΠΈΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ (Π ΠΠ) ΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠ΅ ΡΠΊΡΠ°Π½Ρ Π½Π° ΠΈΡ
ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ²Π»ΡΡΡΡΡ ΠΎΠ΄Π½ΠΈΠΌ ΠΈΠ· ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΡΡΠ΅Π΄ΡΡΠ² ΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ ΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΠΎΡΡΠΈ ΡΠ°Π΄ΠΈΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΡΠ΅Ρ
Π½ΠΈΠΊΠΈ. Π‘ΡΠ΅Π΄ΠΈ ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±ΡΠ°Π·ΠΈΡ
Π ΠΠ ΡΠ²ΠΎΡ Π½ΠΈΡΡ Π·Π°Π½ΠΈΠΌΠ°ΡΡ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ»ΠΈΡΡΠΈΠ»Π΅Π½Π°.
ΠΠ»Ρ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠ½ΡΡ
Π ΠΠ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΠΈΡΡΠΈΠ»Π΅Π½Π°, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅Π³ΠΎ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ Π΄ΠΈΡΠΏΠ΅ΡΡΠ½ΡΠ΅ Π½Π°ΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΠΈ ΠΈ Π°ΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ ΡΠ»Π΅ΠΊΡΡΠΎΠΏΡΠΎΠ²ΠΎΠ΄ΡΡΠΈΠΌΠΈ ΡΠΊΠ°Π½ΡΠΌΠΈ, ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΡΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΡΠΎΠ»ΡΠΈΠ½Ρ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ², ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΡΡ
ΠΎΡΠ»Π°Π±Π»Π΅Π½ΠΈΠ΅ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π‘ΠΠ§-ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎ. ΠΡΠ΅Π½Π΅Π½Ρ ΡΠ°Π΄ΠΈΠΎΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ½ΡΡ
ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠ½ΡΡ
Π ΠΠ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΡΠ°ΡΡΠΎΡ 2,0β27,0 ΠΠΡ ΠΏΡΠΈ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΠΎΠΌ
ΠΏΠ°Π΄Π΅Π½ΠΈΠΈ Π½Π° ΠΎΠ±ΡΠ°Π·Π΅Ρ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ. Π‘ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠ°ΡΡΡΠΎΠ²ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ
ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΠΈΠ·ΡΡΠ΅Π½Π° ΡΡΡΡΠΊΡΡΡΠ° ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠ½ΡΡ
Π ΠΠ.
ΠΠΎ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΈ ΡΠ΅Ρ
Π½ΠΈΠΊΠΎ-ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΊΡΠΈΡΠ΅ΡΠΈΡΠΌ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΠΌΠΈ ΡΡΠ΅Π΄ΡΡΠ²Π°ΠΌΠΈ ΡΠ°Π΄ΠΈΠΎΠ·Π°ΡΠΈΡΡ ΡΠ²Π»ΡΡΡΡΡ Π ΠΠ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½Π½ΡΡ
ΡΠ΅ΡΠΌΠΎΠΏΠ»Π°ΡΡΠΎΠ². Π ΠΠ ΠΎΡΠ½ΠΎΡΡΡΡΡ ΠΊ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π°ΠΌ Π΄Π²ΠΎΠΉΠ½ΠΎΠ³ΠΎ Π½Π°Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΠΈ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ ΠΏΡΠΈ ΡΠΎΠ·Π΄Π°Π½ΠΈΠΈ ΠΌΠ°Π»ΠΎΠ·Π°ΠΌΠ΅ΡΠ½ΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ², Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ Π»Π΅ΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ
Π°ΠΏΠΏΠ°ΡΠ°ΡΠΎΠ².Radioabsorbing materials and electromagnetic screen based on these materials are one of
the effective means of solving electromagnetic safety and electromagnetic compatibility problems
of radioelectronic equipment. Among the variety of radioabsorbing materials loaded
polyethylene based materials hold their own place.
For composite radioabsorbing materials based on polyethylene including various functional
dispersed fillers and reinforced with conducting textiles optimum thickness values of the
samples are specified and also the levels of filling at which the attenuation of microwave radiation
reaches maximum. Radio physical parameters of polymer composite radioabsorbinhg materials
in the range of frequencies of 2,0β27,0 GHz at normal incidence of electromagnetic
wave on a sample are evaluated. Using raster electronic microscopy the structure of composite
radioabsorbing materials have been studied.
Evaluated by technological and technical-economic parameters the most promising means
of radioprotection are radioabsorbing materials based on functionally loaded thermoplastic materials.
Radioabsorbing materials are referred to as double-purpose materials and can be used for
making barely visible objects such as flying apparatuses
Strong Room-Temperature Ferromagnetism of MoS<sub>2</sub> Compound Produced by Defect Generation
Ferromagnetic materials have been attracting great interest in the last two decades due to their application in spintronics devices. One of the hot research areas in magnetism is currently the two-dimensional materials, transition metal dichalcogenides (TMDCs), which have unique physical properties. The origins and mechanisms of transition metal dichalcogenides (TMDCs), especially the correlation between magnetism and defects, have been studied recently. We investigate the changes in magnetic properties with a variation in annealing temperature for the nanoscale compound MoS2. The pristine MoS2 exhibits diamagnetic properties from low-to-room temperature. However, MoS2 compounds annealed at different temperatures showed that the controllable magnetism and the strongest ferromagnetic results were obtained for the 700 Β°C-annealed sample. These magnetizations are attributed to the unpaired electrons of vacancy defects that are induced by annealing, which are confirmed using Raman spectroscopy and electron paramagnetic resonance spectroscopy (EPR)
Effects of Thermal Annealing on Optical and Microscopic Ferromagnetic Properties in InZnP:Ag Nano-Rods
InZnP:Ag nano-rods fabricated by the ion milling method were thermally annealed in the 250~350 °C temperature range and investigated the optimum thermal annealing conditions to further understand the mutual correlation between the optical properties and the microscopic magnetic properties. The formation of InZnP:Ag nano-rods was determined from transmission electron microscopy (TEM), total reflectivity and Raman scattering analyses. The downward shifts of peak position for LO and TO modes in the Raman spectrum are indicative of the production of Ag ion-induced strain during the annealing process of the InZnP:Ag nano-rod samples. The appearance of two emission peaks of both (A0 X) and (e, Ag) in the PL spectrum indicated that acceptor states by Ag diffusion are visible due to the effective incorporation of Ag-creating acceptor states. The binding energy between the acceptor and the exciton measured as a function of temperature was found to be 21.2 meV for the sample annealed at 300 °C. The noticeable MFM image contrast and the clear change in the MFM phase with the scanning distance indicate the formation of the ferromagnetic spin coupling interaction on the surface of InZnP:Ag nano-rods by Ag diffusion. This study suggests that the InZnP:Ag nano-rods should be a potential candidate for the application of spintronic devices
Towards a new class of heavy ion doped magnetic semiconductors for room temperature applications
The article presents, using Bi doped ZnO, an example of a heavy ion doped oxide semiconductor, highlighting a novel p-symmetry interaction of the electronic states to stabilize ferromagnetism. The study includes both ab initio theory and experiments, which yield clear evidence for above room temperature ferromagnetism. ZnBixO1-x thin films are grown using the pulsed laser deposition technique. The room temperature ferromagnetism finds its origin in the holes introduced by the Bi doping and the p-p coupling between Bi and the host atoms. A sizeable magnetic moment is measured by means of x-ray magnetic circular dichroism at the O K-edge, probing directly the spin polarization of the O(2p) states. This result is in agreement with the theoretical predictions and inductive magnetometry measurements. Ab initio calculations of the electronic and magnetic structure of ZnBixO1-x at various doping levels allow to trace the origin of the ferromagnetic character of this material. It appears, that the spin-orbit energy of the heavy ion Bi stabilizes the ferromagnetic phase. Thus, ZnBixO1-x doped with a heavy non-ferromagnetic element, such as Bi, is a credible example of a candidate material for a new class of compounds for spintronics applications, based on the spin polarization of the p states
Room temperature transparent conducting magnetic oxide (TCMO) properties in heavy ion doped oxide semiconductor
Bismuth doped ZnO (ZnBi0.03O0.97) thin films are grown using pulsed laser deposition. The existence of positively charged Bi, absence of metallic zinc and the Zn-O bond formation in Bi doped ZnO are confirmed using X-ray Photoelectron Spectroscopy (XPS). Temperature dependent resistivity and UV-visible absorption spectra show lowest resistivity with 8.44 Γ 10-4 Ξ© cm at 300 K and average transmittance of 93 % in the visible region respectively. The robust ferromagnetic signature is observed at 350 K (7.156 Γ 10-4 emu/g). This study suggests that Bi doped ZnO films should be a potential candidate for spin based optoelectronic applications