66 research outputs found
Effective Conductivity and Magnetic Permeability of Nanostructured Materials in Magnetic Field
The problem of homogenization the nanostructured materials placed in DC magnetic field has been discussed. The experimental data are obtained using metallic superlattices, metal-dielectric thin films and 3D-nanostructured materials. All these materials contain ferro- or ferrimagnetic component. The trans-mission and reflection coefficients were measured on the waves of millimeter waveband. It has been shown that the experimental frequency spectra of the coefficients in zero magnetic field can be described by the effective conductivity and dielectric permittivity. The spectra of ferromagnetic resonance, however, cannot be calculated correctly with the averaged magnetization.
When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3534
Effective Conductivity and Magnetic Permeability of Nanostructured Materials in Magnetic Field
The problem of homogenization the nanostructured materials placed in DC magnetic field has been discussed. The experimental data are obtained using metallic superlattices, metal-dielectric thin films and 3D-nanostructured materials. All these materials contain ferro- or ferrimagnetic component. The trans-mission and reflection coefficients were measured on the waves of millimeter waveband. It has been shown that the experimental frequency spectra of the coefficients in zero magnetic field can be described by the effective conductivity and dielectric permittivity. The spectra of ferromagnetic resonance, however, cannot be calculated correctly with the averaged magnetization.
When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3534
Preparation and structural stability of ordered nanocomposites: opal matrix - lead titanates
The conditions for the formation of nanocomposites based on the basis of lattice packings of SiO[2] nanospheres (opal matrices) with included crystallites of lead titanates (PbTiO[3] and PbTi[3]O[7]) in interspherical nanospacing are considered. For the formation of nanocomposites are used sample opal matrices with dimensions of single-domain regions >=0,1 mm.{3} The diameter of SiO[2] nanospheres was ~260 nm. Obtained nanocomposites volume >2 cm{3} in filling >20% of interspherical nanospacing PbTiO[3], PbTi[3]O[7] crystallites were size of 16-36 nm. Using X-ray diffraction and Raman spectroscopy are studied composition and structural stability when heated nanocomposites to 550Β°C, which allowed the identification of a local phase transition with change of the space group. The dependence of the composition of synthesized materials on the conditions of their preparation is submitted
Stress-induced MICA and MICB molecules in oncology
MICA and MICB molecules, MHC class I chain-related proteins, are expressed on the membranes of damaged, transformed or infected cells. These glycoproteins bind to the NKG2D receptor of NK cells, resulting in their activation and cytotoxic response against MICA- and/or MICB-expressing cells. Expression of NKG2D receptor ligands allows the elimination of tumor and damaged cells. Soluble forms of MICA/B proteins are produced as a result of protein cleavage. Binding of soluble ligands to NKG2D receptors causes their internalization and degradation, leading to a decrease in NK cell activity. Malignant growth of gastrointestinal tissues, pancreas, liver, kidney, lung, skin, and blood cancers is accompanied by increased concentration of soluble MICA/B in blood plasma of the patients. High concentrations of these proteins are associated with lower overall and recurrence-free survival in the patients. Soluble MICA/B contribute to immunosuppressive tumor microenvironment, and increase in their plasma contents is considered an index of tumor escape from the immune surveillance. The role of MICA/B protein changes during carcinogenesis is also under studies. At the early stage of tumor formation, these proteins contribute to activation of NK cells and elimination of transformed cells, whereas, at the later stage of this process, the increased production of its soluble forms leads to a decrease in anti-tumor activity of NK cells. Standard cancer treatment, such as chemotherapy, is accompanied by increased density of these molecules on the tumor cells. In addition, preclinical studies show that inhibition of MICA/B shedding with antibodies or their derivatives may also promote the anti-tumor activity of NK cells. This review summarizes basic information on the biology of MICA/B molecules, their expression by normal and transformed cells, elucidates the role of these molecules in anti-tumor immune surveillance, and provides information on the potential use of MICA/B in diagnosis and therapy of malignant diseases
ΠΠΠΠ£Π§ΠΠΠΠ Π Π€ΠΠΠΠ§ΠΠ‘ΠΠΠ Π‘ΠΠΠΠ‘Π’ΠΠ ΠΠΠΠΠΠΠ«Π₯ ΠΠΠ’Π ΠΠ¦ Π‘ ΠΠΠΠΠ§ΠΠ‘Π’ΠΠ¦ΠΠΠ ΠΠΠ‘ΠΠΠΠ Fe Π Ti
The article considers specific features of the formation of nanocomposites based on the lattice packing of SiO2 nanospheres (opal matrices) with clusters of titanium and iron compounds (FeTiO3, FeTi2O5, TiO2, Fe2O3) embedded into nanopores between spheres. For the formation of the nanocomposites samples of opal matrices with the sizes of single-domain regions > 0.1 mm3 were used. The diameter of the SiO2 nanospheres was ~260 nm. Nanocomposites with the volume > 1 cm3 and 10-15% of interspherical nanospacing filled by crystallites of titanium and iron compounds were obtained. The composition and structure of the nanocomposites were studied by electron microscopy, X-ray diffraction and Raman spectroscopy. The dependence of the composition of the synthesized materials on the conditions of their preparation is shown. Results of measurements of the frequency dependences (within the range 1 MHz - 3 GHz) of the magnetic and dielectric characteristics of the obtained nanostructures are presented. Hysteresis loops were studied for the obtained samples.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π½Π°Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ΅ΡΠ΅ΡΡΠ°ΡΡΡ
ΡΠΏΠ°ΠΊΠΎΠ²ΠΎΠΊ Π½Π°Π½ΠΎΡΡΠ΅Ρ SiO2 (ΠΎΠΏΠ°Π»ΠΎΠ²ΡΡ
ΠΌΠ°ΡΡΠΈΡ), ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
Π² ΠΌΠ΅ΠΆΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»ΠΎΡΡΡΡ
ΠΊΠ»Π°ΡΡΠ΅ΡΡ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΡΠΈΡΠ°Π½Π° ΠΈ ΠΆΠ΅Π»Π΅Π·Π° (FeTiO3, FeTi2O5, TiO2, Fe2O3). ΠΠ»Ρ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π½Π°Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΎΠ² ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈ ΠΎΠ±ΡΠ°Π·ΡΡ ΠΎΠΏΠ°Π»ΠΎΠ²ΡΡ
ΠΌΠ°ΡΡΠΈΡ Ρ ΡΠ°Π·ΠΌΠ΅ΡΠ°ΠΌΠΈ ΠΌΠΎΠ½ΠΎΠ΄ΠΎΠΌΠ΅Π½Π½ΡΡ
ΠΎΠ±Π»Π°ΡΡΠ΅ΠΉ > 0,1 ΠΌΠΌ3, Π΄ΠΈΠ°ΠΌΠ΅ΡΡ Π½Π°Π½ΠΎΡΡΠ΅Ρ SiO2 ΡΠΎΡΡΠ°Π²Π»ΡΠ» ~260 Π½ΠΌ. ΠΠΎΠ»ΡΡΠ΅Π½Ρ Π½Π°Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΡ ΠΎΠ±ΡΠ΅ΠΌΠΎΠΌ > 1 ΡΠΌ3 Ρ Π·Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠ΅ΠΌ 10-15% ΠΎΠ±ΡΠ΅ΠΌΠ° ΠΌΠ΅ΠΆΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»ΠΎΡΡΠ΅ΠΉ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ°ΠΌΠΈ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΡΠΈΡΠ°Π½Π° ΠΈ ΠΆΠ΅Π»Π΅Π·Π°. ΠΠ·ΡΡΠ΅Π½Ρ ΡΠΎΡΡΠ°Π² ΠΈ ΡΡΡΠΎΠ΅Π½ΠΈΠ΅ Π½Π°Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΎΠ² Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠΌΠ΅ΡΡΠΈΠΈ ΠΈ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ ΡΠ²Π΅ΡΠ°. ΠΠΎΠΊΠ°Π·Π°Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΡΠΎΡΡΠ°Π²Π° ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π²Π΅ΡΠ΅ΡΡΠ² ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΈΡ
ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ ΡΠ°ΡΡΠΎΡΠ½ΡΡ
(Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ 1 ΠΠΡ - 3 ΠΠΡ) Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠ΅ΠΉ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΈ Π΄ΠΈΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡ. ΠΡΠΎΠ²Π΅Π΄Π΅Π½Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠ΅ΡΠ΅Π»Ρ Π³ΠΈΡΡΠ΅ΡΠ΅Π·ΠΈΡΠ° Π΄Π»Ρ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΎΠ±ΡΠ°Π·ΡΠΎΠ²
Π‘Π’Π ΠΠΠΠΠ Π ΠΠΠΠΠΠΠ’Π ΠΠ§ΠΠ‘ΠΠΠ Π‘ΠΠΠΠ‘Π’ΠΠ ΠΠΠΠΠΠΠΠΠΠΠΠ’ΠΠ: ΠΠΠΠΠΠΠ«Π ΠΠΠ’Π ΠΠ¦Π« - ΠΠΠ‘ΠΠΠ« Π’ΠΠ’ΠΠΠ Π Π’ΠΠ’ΠΠΠΠ’Π« Π ΠΠΠΠΠΠΠΠΠΠ¬ΠΠ«Π₯ ΠΠΠΠΠΠΠ’ΠΠ
The conditions for the formation of nanocomposites based on the basis of lattice packings SiO2 nanospheres (opal matrices) with included clusters of crystalline phase of titanium oxide (TiO2 and TiO) and rare-earth titanates of the general formula R2TiO5 or R2Ti2O7, where R - Er, Dy, Gd, Pr, Tb and Yb in interspherical nanospacing are considered. The composition and structure of the nanocomposites studied electron microscopy, X-ray diffraction and Raman spectroscopy. Results of measuring of the frequency dependences of real and imaginary components of the permittivity and microwave conductivity (ranging 10-2-1012 Hz) obtained nanostructures are viewed.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π½Π°Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ΅ΡΠ΅ΡΡΠ°ΡΡΡ
ΡΠΏΠ°ΠΊΠΎΠ²ΠΎΠΊ Π½Π°Π½ΠΎΡΡΠ΅Ρ SiO2 (ΠΎΠΏΠ°Π»ΠΎΠ²ΡΡ
ΠΌΠ°ΡΡΠΈΡ), ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
Π² ΠΌΠ΅ΠΆΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»ΠΎΡΡΡΡ
ΠΊΠ»Π°ΡΡΠ΅ΡΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°Π· ΠΎΠΊΡΠΈΠ΄ΠΎΠ² ΡΠΈΡΠ°Π½Π° (TiO2 ΠΈ TiO) ΠΈ ΡΠΈΡΠ°Π½Π°ΡΠΎΠ² ΡΠ΅Π΄ΠΊΠΎΠ·Π΅ΠΌΠ΅Π»ΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΡΠΎΡΡΠ°Π²Π° R2TiO5 ΠΈΠ»ΠΈ R2Ti2O7, Π³Π΄Π΅ R - Er, Dy, Gd, Pr, Tb ΠΈ Yb. ΠΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠΌΠ΅ΡΡΠΈΠΈ ΠΈ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ ΡΠ²Π΅ΡΠ° ΠΈΠ·ΡΡΠ΅Π½Ρ ΡΠΎΡΡΠ°Π² ΠΈ ΡΡΡΠΎΠ΅Π½ΠΈΠ΅ Π½Π°Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΎΠ². ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ ΡΠ°ΡΡΠΎΡΠ½ΡΡ
Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠ΅ΠΉ Π΄Π΅ΠΉΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΠΈ ΠΌΠ½ΠΈΠΌΠΎΠΉ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ Π΄ΠΈΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠΎΠ½ΠΈΡΠ°Π΅ΠΌΠΎΡΡΠΈ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΌΠΈΠΊΡΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΡΡΠΈ (Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ 10-2-1012 ΠΡ) ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡ
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