23 research outputs found
Contribution of magnetic aftereffect and induction transition characteristics of basalts from the Vitim plateau
To study magnetic aftereffect (magnetic viscosity) with its manifestations making difficulties for interpretation of the data of transitional processes, comprehensive experimental studies of samples have been conducted, which characterize the upper rock mass of the Vitim basaltic plateau. An attempt to reveal the character of distribution of magnetically viscous rocks within volcano-sedimentary succession of strata has been made and to find out which ferromagnetic particles display the effect of magnetic viscosity on the inductive transient response. It has been shown that in time-domain measurements with inductive systems the greatest contribution of magnetic viscosity effect is brought by the most fresh, unchanged rocks. Magnetic viscosity effect is mainly caused by super-paramagnetic grains of low-titanic titanomagnetite, close to pure magnetite with rather narrow grain-size interval (most probably 0.0254-0.029 mm). As for the smaller superparamagnetic grains, the contribution of relaxation of their magnetization to inductive transient responses is approximately 3 times lower. Possible criteria of diagnostics of superparamagnetic particles of different size are proposed on the base of petro-magnetic data
New data on the metallogeny and deep structure of the Kirovograd Polymetal ore district (Ukrainian Shield)
Structural and petrological localization conditions and age relationships of uranium and gold deposits are discussed. A specific type of adulariachlorite wallrock alteration is found to be associated with sulfidegold mineralization. The relation between uranium, gold, lithium deposits and the topography of K2 and M surfaces are described. A 3 D seismic model of the Kirovograd ore district is suggested
ΠΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Π½Ρ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΈΡ Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΠ΅ΠΉ ΠΊΠΎΠ΅ΡΡΡΡΡΠ½ΡΠ° ΠΏΠΎΠ³Π»ΠΈΠ½Π°Π½Π½Ρ Π² ΡΠΎΠ½ΠΊΠΈΡ ΠΏΠ»ΡΠ²ΠΊΠ°Ρ Π³ΡΠ΄ΡΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΏΠΎΡΡΡΠΉΠ½ΠΎΠ³ΠΎ ΡΠΎΡΠΎΡΡΡΡΠΌΡ Π· ΠΌΠΎΠ΄ΡΠ»ΡΠΎΠ²Π°Π½ΠΈΠΌ Π·Π±ΡΠ΄ΠΆΠ΅Π½Π½ΡΠΌ
Spectral dependences of absorption coefficient in thin films of amorphous hydrogenated silicon are investigated. Silicon films were obtained by decomposition of monosilane and hydrogen mixture under hydrogen portion, corresponding to conditions of the beginning of nanocrystalline phase formation in structure of films. A new modification of the constant photocurrent method, based on the modulation of the exciting light flux, is developed and used to measure the spectral dependence of the absorption coefficient. The effect of illumination of different duration on films absorption spectra, measured by the proposed method, is investigated. According to the study of a-Si:H films, obtained under conditions corresponding to the beginning of formation of the crystalline phase, we can assume the presence of silicon nanocrystals in structure of the films and nanocrystals influence on the optical properties of a-Si:H.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΡ Π² ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΊΠ°Ρ
Π°ΠΌΠΎΡΡΠ½ΠΎΠ³ΠΎ Π³ΠΈΠ΄ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΡΠΌΠ΅ΡΠΈ ΠΌΠΎΠ½ΠΎΡΠΈΠ»Π°Π½Π° ΠΈ Π²ΠΎΠ΄ΠΎΡΠΎΠ΄Π° ΠΏΡΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ Π΄ΠΎΠ»Π΅ Π²ΠΎΠ΄ΠΎΡΠΎΠ΄Π° Π² Π³Π°Π·ΠΎΠ²ΠΎΠΉ ΡΠΌΠ΅ΡΠΈ, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠ΅ΠΉ ΡΡΠ»ΠΎΠ²ΠΈΡΠΌ Π½Π°ΡΠ°Π»Π° ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π½Π°Π½ΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ°Π·Ρ Π² ΡΡΡΡΠΊΡΡΡΠ΅ ΠΏΠ»Π΅Π½ΠΎΠΊ. ΠΠ»Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠ΅ΠΉ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΡ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ ΠΌΠΎΠ΄ΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠ³ΠΎ ΡΠΎΡΠΎΡΠΎΠΊΠ°, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΠΉ Π½Π° ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π²ΠΎΠ·Π±ΡΠΆΠ΄Π°ΡΡΠ΅Π³ΠΎ ΡΠ²Π΅ΡΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΡΠΎΠΊΠ°. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΎΡΠ²Π΅ΡΠ΅Π½ΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠΉ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ Π½Π° ΡΠΏΠ΅ΠΊΡΡΡ ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΡ ΠΏΠ»Π΅Π½ΠΎΠΊ, ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠ»Π΅Π½ΠΎΠΊ a-Si:H, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΡ
Π½Π°ΡΠ°Π»Ρ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ°Π·Ρ, ΠΌΠΎΠΆΠ½ΠΎ ΠΏΡΠ΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠΈΡΡ Π½Π°Π»ΠΈΡΠΈΠ΅ Π² ΡΡΡΡΠΊΡΡΡΠ΅ ΠΏΠ»Π΅Π½ΠΎΠΊ Π½Π°Π½ΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, Π²Π»ΠΈΡΡΡΠΈΡ
Π½Π° ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° a-Si:H.ΠΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½ΠΎ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½Ρ Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ ΠΊΠΎΠ΅ΡΡΡΡΡΠ½ΡΠ° ΠΏΠΎΠ³Π»ΠΈΠ½Π°Π½Π½Ρ Π² ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»ΡΠ²ΠΊΠ°Ρ
Π°ΠΌΠΎΡΡΠ½ΠΎΠ³ΠΎ Π³ΡΠ΄ΡΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΡΡ, ΠΎΡΡΠΈΠΌΠ°Π½ΠΈΡ
ΡΠΎΠ·ΠΊΠ»Π°Π΄Π°Π½Π½ΡΠΌ ΡΡΠΌΡΡΡ ΠΌΠΎΠ½ΠΎΡΡΠ»Π°Π½Π° Ρ Π²ΠΎΠ΄Π½Ρ ΠΏΡΠΈ Π²ΡΠ΄Π½ΠΎΡΠ½ΡΠΉ ΡΠ°ΡΡΡΡ Π²ΠΎΠ΄Π½Ρ Π² Π³Π°Π·ΠΎΠ²ΡΠΉ ΡΡΠΌΡΡΡ, ΡΠΎ Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π°Ρ ΡΠΌΠΎΠ²Π°ΠΌ ΠΏΠΎΡΠ°ΡΠΊΡ ΡΠΎΡΠΌΡΠ²Π°Π½Π½Ρ Π½Π°Π½ΠΎΠΊΡΠΈΡΡΠ°Π»ΡΡΠ½ΠΎΡ ΡΠ°Π·ΠΈ Π² ΡΡΡΡΠΊΡΡΡΡ ΠΏΠ»ΡΠ²ΠΎΠΊ. ΠΠ»Ρ Π²ΠΈΠΌΡΡΡΠ²Π°Π½Π½Ρ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΈΡ
Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΠ΅ΠΉ ΠΊΠΎΠ΅ΡΡΡΡΡΠ½ΡΠ° ΠΏΠΎΠ³Π»ΠΈΠ½Π°Π½Π½Ρ Π·Π°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΈΠΉ Ρ Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½ΠΈΠΉ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠΎΠ²Π°Π½ΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΏΠΎΡΡΡΠΉΠ½ΠΎΠ³ΠΎ ΡΠΎΡΠΎΡΡΡΡΠΌΡ, Π·Π°ΡΠ½ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π° ΠΌΠΎΠ΄ΡΠ»ΡΡΡΡ Π·Π±ΡΠ΄Π»ΠΈΠ²ΠΎΠ³ΠΎ ΡΠ²ΡΡΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΡΠΎΠΊΡ. ΠΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½ΠΎ Π²ΠΏΠ»ΠΈΠ² ΠΎΡΠ²ΡΡΠ»Π΅Π½Π½Ρ ΡΡΠ·Π½ΠΎΡ ΡΡΠΈΠ²Π°Π»ΠΎΡΡΡ Π½Π° ΡΠΏΠ΅ΠΊΡΡΠΈ ΠΏΠΎΠ³Π»ΠΈΠ½Π°Π½Π½Ρ ΠΏΠ»ΡΠ²ΠΎΠΊ, Π²ΠΈΠΌΡΡΡΠ½ΠΈΡ
Π·Π°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΈΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ.ΠΠ° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌΠΈ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Π½Ρ ΠΏΠ»ΡΠ²ΠΎΠΊ a-Si: H, ΠΎΡΡΠΈΠΌΠ°Π½ΠΈΡ
Π² ΡΠΌΠΎΠ²Π°Ρ
, ΡΠΎ Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π°ΡΡΡ ΠΏΠΎΡΠ°ΡΠΊΡ ΡΠΎΡΠΌΡΠ²Π°Π½Π½Ρ ΠΊΡΠΈΡΡΠ°Π»ΡΡΠ½ΠΎΡ ΡΠ°Π·ΠΈ, ΠΌΠΎΠΆΠ½Π° ΠΏΡΠΈΠΏΡΡΡΠΈΡΠΈ Π½Π°ΡΠ²Π½ΡΡΡΡ Ρ ΡΡΡΡΠΊΡΡΡΡ ΠΏΠ»ΡΠ²ΠΎΠΊ Π½Π°Π½ΠΎΠΊΡΠΈΡΡΠ°Π»ΡΠ² ΠΊΡΠ΅ΠΌΠ½ΡΡ, ΡΠΎ Π²ΠΏΠ»ΠΈΠ²Π°ΡΡΡ Π½Π° ΠΎΠΏΡΠΈΡΠ½Ρ Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΡ a-Si: H