364 research outputs found
Ionospheric effects during first 2 hours after the Chelyabinsk meteorite impact
This paper presents the analysis of ionospheric effects in the region close
to the Chelyabinsk meteorite explosion at 03:20UT 2013 February 15 from the
Institute of Solar-Terrestrial Physics of Siberian Branch of Russian Academy of
Sciences (ISTP SB RAS) EKB radar data, and from the Institute of Geophysics of
Ural Branch of Russian Academy of Sciences (IG UB RAS) PARUS ionosonde data.
Both instruments are located within the IG UB RAS Arti Observatory
approximately 200 km northward from the estimated explosion site. According to
the data obtained, the ionospheric disturbance caused by the meteorite flyby,
explosion, and impact had high dynamics and amplitude. However, it obviously
did not lead to a variation in the ionosphere mean parameters in the region
above the disturbance center during the first 2 hours. Essential effects,
however, were observed at more than 100-200 km from the explosion site and
farther up to 1500 km.Comment: 30 pages, 15 figures, submitted to JAST
Superhyperfine interactions in Ce3+ doped LiYF4 crystal: ENDOR measurements
The first observation of the resolved Mims electron-nuclear double resonance
(ENDOR) spectra from the nearby and remote nuclei of 19F and 7Li nuclei on
impurity Ce3+ ions in LiYF4 crystal is reported. It shows that LiYF4:Ce3+
system can be exploited as a convenient matrix for performing spin
manipulations and adjusting quantum computation protocols while ENDOR technique
could be used for the investigation of electron-nuclear interaction with all
the nuclei of the system and exploited for the electron-nuclear spin
manipulations.Comment: 4 pages, 2 figures, 1 Table. Reported on Theor-2017 (Kazan, Russia)
Conferenc
ΠΠΎΠ²ΡΠ΅ ΠΏΠΎΠ΄Ρ ΠΎΠ΄Ρ ΠΊ ΡΡΠ°Π½Π΄Π°ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΡΠ°Π²Ρ ΠΌΠΎΠ½Π°ΡΠ΄Ρ Π΄ΡΠ΄ΡΠ°ΡΠΎΠΉ
Objectives. The Monarda fistulosa herb of the Lamiaceae family is particularly interesting among essential oils from medicinal plants that have a wide spectrum of pharmacological activities. However, information regarding some of its flavonoids, which are found in the essential oil, is controversial. Inaccuracies in identification of the chemical composition of the herb have led to several different standardization approaches, which are cumbersome. To establish a uniform classification, here, we present confirmation for new approaches for the standardization of the Monarda fistulosa herb. Methods. Silica gel column chromatography was used to extract the flavonoids. Identification was based on ultraviolet spectroscopy, nuclear magnetic resonance spectroscopy, mass spectrometry, and acidic hydrolysis. The quality of the proposed quantitation methodology for total flavonoids was assessed by differential spectrophotometry at 394 nm, in isorhoifolin equivalent.Results. We have verified new approaches for the standardization of the Monarda fistulosa herb. The approaches can determine the authenticity of the herb by detecting monoterpene phenols and flavonoids that have diagnostic value. We also developed a technique for quantitation of the total flavonoids. Conclusions. We investigated the possibility of establishing the authenticity of the Monarda fistulosa herb based on the diagnostically significant flavonoids, isorhoifolin and linarin.Π¦Π΅Π»ΠΈ. Π‘ΡΠ΅Π΄ΠΈ ΡΡΠΈΡΠΎΠΌΠ°ΡΠ»ΠΈΡΠ½ΡΡ
Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΡΡ
ΡΠ°ΡΡΠ΅Π½ΠΈΠΉ, ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΡ
ΡΠΈΡΠΎΠΊΠΈΠΌ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌ ΡΠ°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ, ΠΎΡΠΎΠ±ΡΠΉ ΠΈΠ½ΡΠ΅ΡΠ΅Ρ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΡΠ°Π²Π° ΠΌΠΎΠ½Π°ΡΠ΄Ρ Π΄ΡΠ΄ΡΠ°ΡΠΎΠΉ (Monarda fistulosa) ΡΠ΅ΠΌΠ΅ΠΉΡΡΠ²Π° Π―ΡΠ½ΠΎΡΠΊΠΎΠ²ΡΡ
. ΠΠ΄Π½Π°ΠΊΠΎ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΡ ΠΎ Π½Π΅ΠΊΠΎΡΠΎΡΡΡ
ΡΠ»Π°Π²ΠΎΠ½ΠΎΠΈΠ΄Π°Ρ
, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
ΡΡ Π² Π½Π΅ΠΉ Π½Π°ΡΡΠ΄Ρ Ρ ΡΡΠΈΡΠ½ΡΠΌ ΠΌΠ°ΡΠ»ΠΎΠΌ, Π½ΠΎΡΠΈΡ ΠΏΡΠΎΡΠΈΠ²ΠΎΡΠ΅ΡΠΈΠ²ΡΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅Ρ. ΠΠ΅ΡΠΎΡΠ½ΠΎΡΡΠΈ, Π²ΡΡΠ²Π»Π΅Π½Π½ΡΠ΅ Π² ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΈ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΎΡΡΠ°Π²Π° ΡΡΠ°Π²Ρ, ΡΡΠ°Π½ΠΎΠ²ΡΡΡΡ ΠΏΡΠΈΡΠΈΠ½ΠΎΠΉ ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ΠΎΠ² ΠΊ ΡΡΠ°Π½Π΄Π°ΡΡΠΈΠ·Π°ΡΠΈΠΈ, ΡΡΠΎ ΡΠΎΠ·Π΄Π°Π΅Ρ ΡΡΡΠ΄Π½ΠΎΡΡΠΈ. ΠΠ»Ρ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ Π΅Π΄ΠΈΠ½ΠΎΠΎΠ±ΡΠ°Π·ΠΈΡ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π² Π΄Π°Π½Π½ΠΎΠΉ ΡΠ°Π±ΠΎΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΎ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠ΅ Π½ΠΎΠ²ΡΡ
, ΡΠ°Π½Π΅Π΅ Π½Π΅ ΠΏΡΠΈΠΌΠ΅Π½ΡΠ²ΡΠΈΡ
ΡΡ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ΠΎΠ² ΠΊ ΡΡΠ°Π½Π΄Π°ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΡΠ°Π²Ρ ΠΌΠΎΠ½Π°ΡΠ΄Ρ Π΄ΡΠ΄ΡΠ°ΡΠΎΠΉ. ΠΠ΅ΡΠΎΠ΄Ρ. ΠΠ»Ρ ΡΠΊΡΡΡΠ°ΠΊΡΠΈΠΈ ΡΠ»Π°Π²ΠΎΠ½ΠΎΠΈΠ΄ΠΎΠ² ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈ ΠΊΠΎΠ»ΠΎΠ½ΠΎΡΠ½ΡΡ Ρ
ΡΠΎΠΌΠ°ΡΠΎΠ³ΡΠ°ΡΠΈΡ Π½Π° ΡΠΈΠ»ΠΈΠΊΠ°Π³Π΅Π»Π΅. ΠΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ Π΄Π°Π½Π½ΡΡ
ΡΠ»ΡΡΡΠ°ΡΠΈΠΎΠ»Π΅ΡΠΎΠ²ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΡΠ΄Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠ° ΠΈ ΠΌΠ°ΡΡ-ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΠΈ, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΊΠΈΡΠ»ΠΎΡΠ½ΠΎΠ³ΠΎ Π³ΠΈΠ΄ΡΠΎΠ»ΠΈΠ·Π°. ΠΡΠ΅Π½ΠΊΡ ΠΊΠ°ΡΠ΅ΡΡΠ²Π° ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΠΌΠΌΡ ΡΠ»Π°Π²ΠΎΠ½ΠΎΠΈΠ΄ΠΎΠ² ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΠΈ ΠΏΡΠΈ 394 Π½ΠΌ Π² ΠΏΠ΅ΡΠ΅ΡΡΠ΅ΡΠ΅ Π½Π° ΠΈΠ·ΠΎΡΠΎΠΈΡΠΎΠ»ΠΈΠ½. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Ρ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Ρ ΠΊ ΡΡΠ°Π½Π΄Π°ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΡΠ°Π²Ρ ΠΌΠΎΠ½Π°ΡΠ΄Ρ Π΄ΡΠ΄ΡΠ°ΡΠΎΠΉ, Π·Π°ΠΊΠ»ΡΡΠ°ΡΡΠΈΠ΅ΡΡ Π² ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ Π΅Π΅ ΠΏΠΎΠ΄Π»ΠΈΠ½Π½ΠΎΡΡΠΈ ΠΏΡΡΠ΅ΠΌ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ ΠΌΠΎΠ½ΠΎΡΠ΅ΡΠΏΠ΅Π½ΠΎΠ²ΡΡ
ΡΠ΅Π½ΠΎΠ»ΠΎΠ² ΠΈ ΡΠ»Π°Π²ΠΎΠ½ΠΎΠΈΠ΄ΠΎΠ², ΠΈΠΌΠ΅ΡΡΠΈΡ
Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅. Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π° ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΠΌΠΌΡ ΡΠ»Π°Π²ΠΎΠ½ΠΎΠΈΠ΄ΠΎΠ².ΠΡΠ²ΠΎΠ΄Ρ. ΠΠ·ΡΡΠ΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΏΠΎΠ΄Π»ΠΈΠ½Π½ΠΎΡΡΠΈ ΡΡΠ°Π²Ρ ΠΌΠΎΠ½Π°ΡΠ΄Ρ Π΄ΡΠ΄ΡΠ°ΡΠΎΠΉ, ΠΈΡΡ
ΠΎΠ΄Ρ ΠΈΠ· Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·Π½Π°ΡΠΈΠΌΡΡ
ΡΠ»Π°Π²ΠΎΠ½ΠΎΠΈΠ΄ΠΎΠ² β ΠΈΠ·ΠΎΡΠΎΠΈΡΠΎΠ»ΠΈΠ½Π° ΠΈ Π»ΠΈΠ½Π°ΡΠΈΠ½Π°
Temperature dependence of the EPR linewidth of Yb3+ - ions in Y0.99Yb0.01Ba2Cu3OX compounds: Evidence for an anomaly near TC
Electron paramagnetic resonance experiments on doped Yb3+ ions in YBaCuO
compounds with different oxygen contents have been made. We have observed the
strong temperature dependence of the EPR linewidth in the all investigated
samples caused by the Raman processes of spin-lattice relaxation. The
spin-lattice relaxation rate anomaly revealed near TC in the superconducting
species can be assigned to the phonon density spectrum changesComment: 10 pages, 4 figures Renewed versio
Inhomogeneity of the intrinsic magnetic field in superconducting YBa2Cu3OX compounds as revealed by rare-earth EPR-probe
X-band electron paramagnetic resonance on doped Er3+ and Yb3+ ions in
Y0.99(Yb,Er)0.01Ba2Cu3OX compounds with different oxygen contents in the wide
temperature range (4-120)K have been made. In the superconducting species, the
strong dependencies of the linewidth and resonance line position from the sweep
direction of the applied magnetic field are revealed at the temperatures
significantly below TC. The possible origins of the observed hysteresis are
analyzed. Applicability of the presented EPR approach to extract information
about the dynamics of the flux-line lattice and critical state parameters
(critical current density, magnetic penetration depth, and characteristic
spatial scale of the inhomogeneity) is discussedComment: 17 pages, 5 Figures. Renewed versio
Superhyperfine structure of the ESR spectra of Gd<sup>3+</sup> impurity ions in LiYF<inf>4</inf> double fluoride
Β© 2017, Pleiades Publishing, Ltd.Electron spin resonance spectra of Gd3+ ions forming a small (~0.0001 at %) impurity in a LiYF4 single crystal have been investigated in a wide temperature range from liquid helium to room temperature. A number of the fine-structure components of the spectrum exhibit a pronounced superhyperfine structure depending on the orientation of the external magnetic field with respect to the crystallographic axes. The superhyperfine structure was not observed in earlier ESR studies of double fluorides with a Gd3+ impurity
Superhyperfine structure of the EPR spectra of impurity ions in the LiYF4 : Nd3+ system doped by 143Nd isotopes
Β© 2015, Pleiades Publishing, Ltd. Results of measuring the EPR spectra in the LiYF4: Nd3+ system doped by 143Nd isotopes with the nuclear spin I = 7/2 have been presented. We have succeeded to observe superhyperfine splitting of the EPR spectra of the samples under investigation at the orientation of the magnetic field B along the symmetry axis c of the crystal and at B β₯ c on the lines corresponding to both even neodymium isotopes and 143Nd
ζΈθ© ε «η°ι倫θ γζΆθ²»η¨γ―γγ―γγγγͺγγ
The superhyperfine structure of the EPR spectra of impurity Nd3+ and U3+ ions in LiYF4, LiLuF4, and LiTmF4 double-fluoride single crystals has been observed and discussed. In LiYF4: Nd (g{pipe} = 1. 987, gβ₯ = 2. 554) and LiTmF4: Nd, the superhyperfine structure is observed at the orientation of the external magnetic field B in parallel to the c axis of the crystals and consists of nine components with a splitting of ~15. 4 MHz. In LiYF4: U (g{pipe} = 1. 149, gβ₯ = 2. 508) and LiLuF4: U, the superhyperfine structure is observed at both B {pipe} c and B β₯ c and consists of nine and eleven components, respectively, with a splitting of ~21. 5MHz. It should be noted that the resolution of the superhyperfine structure of the EPR spectrum of LiLuF4: U3+ becomes significantly higher with a deviation from the orientation B β₯ c. Β© 2011 Pleiades Publishing, Ltd
Enhanced superhyperfine structure of the EPR spectra of a U3+ ion introduced into the Van Vleck paramagnet LiTmF4
The observation of the superhyperfine structure (SHFS) in EPR spectra due to enhanced nuclear magnetism is reported. The X-band spectrum of a U 3+ ion introduced into the Van Vleck paramagnet LiTmF4 is measured in the temperature range of 5-20 K and compared with the spectra of LiLuF4:U3+ and LiYF4:U3+ single crystals. The spectra reveal well-resolved and strikingly different SHFS. The SHFS of Li(Lu, Y)F4:U3+ is due to the fluorine ions forming the nearest surroundings of the U3+ ion. The main contribution to the SHFS of the U3+ spectrum in LiTmF4 comes from the Tm3+ ions with a highly enhanced nuclear gyromagnetic tensor. Β© 2008 Pleiades Publishing, Ltd
Superhyperfine structure of the EPR spectra of Nd3+ and U3+ ions in LiRF4 (R = Y, Lu, Tm) double fluorides
The superhyperfine structure of the EPR spectra of impurity Nd3+ and U3+ ions in LiYF4, LiLuF4, and LiTmF4 double-fluoride single crystals has been observed and discussed. In LiYF4: Nd (g{pipe} = 1. 987, gβ₯ = 2. 554) and LiTmF4: Nd, the superhyperfine structure is observed at the orientation of the external magnetic field B in parallel to the c axis of the crystals and consists of nine components with a splitting of ~15. 4 MHz. In LiYF4: U (g{pipe} = 1. 149, gβ₯ = 2. 508) and LiLuF4: U, the superhyperfine structure is observed at both B {pipe} c and B β₯ c and consists of nine and eleven components, respectively, with a splitting of ~21. 5MHz. It should be noted that the resolution of the superhyperfine structure of the EPR spectrum of LiLuF4: U3+ becomes significantly higher with a deviation from the orientation B β₯ c. Β© 2011 Pleiades Publishing, Ltd
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