412 research outputs found

    Lifetime of Gapped Excitations in a Collinear Quantum Antiferromagnet

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    We demonstrate that local modulations of magnetic couplings have a profound effect on the temperature dependence of the relaxation rate of optical magnons in a wide class of antiferromagnets in which gapped excitations coexist with acoustic spin waves. In a two-dimensional collinear antiferromagnet with an easy-plane anisotropy, the disorder-induced relaxation rate of the gapped mode, Gamma_imp=Gamma_0+A(TlnT)^2, greatly exceeds the magnon-magnon damping, Gamma_m-m=BT^5, negligible at low temperatures. We measure the lifetime of gapped magnons in a prototype XY antiferromagnet BaNi2(PO4)2 using a high-resolution neutron-resonance spin-echo technique and find experimental data in close accord with the theoretical prediction. Similarly strong effects of disorder in the three-dimensional case and in noncollinear antiferromagnets are discussed.Comment: 4.5 pages + 2.5 pages supplementary material, published versio

    Crystal structure of mixed fluorites Ca(1-x)Sr(x)F(2) and Sr(1-x)Ba(x)F(2) and luminescence of Eu(2+) in the crystals

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    Within the framework of the virtual crystal method implemented in the shell model and pair potential approximation the crystal structure of mixed fluorites Ca(1-x)Sr(x)F(2) and Sr(1-x)Ba(x)F(2) has been calculated. The impurity center Eu(2+) and the distance Eu(2+)-F in this crystals have been also calculated. The low level position of excited 4f65d configuration of the Eu(2+) ion has been expressed using phenomenological dependence on distance E(2+)-F. The dependences of Stokes shift and Huang-Rhys factor on concentration x have been received for yellow luminescence in Sr(1-x)Ba(x)F(2):Eu(2+). The value x, for which the eg -level of Eu(2+) ion will be in conduction band in Sr(1-x)Ba(x)F(2):Eu(2+) has been calculated.Comment: 8 pages, 3 figures. The manuscript is sent to journal 'Physics of the solid state'. The results will be submitted on inernational conference SCINTMAT'2002 in oral session (june,20-22,2002,Ekaterinburg,Russia). Corresponding author e-mail: [email protected]

    Instability of antiferromagnetic magnons in strong fields

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    We predict that spin-waves in an ordered quantum antiferromagnet (AFM) in a strong magnetic field become unstable with respect to spontaneous two-magnon decays. At zero temperature, the instability occurs between the threshold field Hβˆ—H^* and the saturation field HcH_c. As an example, we investigate the high-field dynamics of a Heisenberg antiferromagnet on a square lattice and show that the single-magnon branch of the spectrum disappears in the most part of the Brillouin zone.Comment: RevTeX, 4 pages, 3 figures, accepted to PR

    Holes in the t-J_z model: a thorough study

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    The t-J_z model is the strongly anisotropic limit of the t-J model which captures some general properties of the doped antiferromagnets (AF). The absence of spin fluctuations simplifies the analytical treatment of hole motion in an AF background and allows us to calculate the single- and two-hole spectra with high accuracy using regular diagram technique combined with real-space approach. At the same time, numerical studies of this model via exact diagonalization (ED) on small clusters show negligible finite size effects for a number of quantities, thus allowing a direct comparison between analytical and numerical results. Both approaches demonstrate that the holes have tendency to pair in the p- and d-wave channels at realistic values of t/J. The interactions leading to pairing and effects selecting p and d waves are thoroughly investigated. The role of transverse spin fluctuations is considered using perturbation theory. Based on the results of the present study, we discuss the pairing problem in the realistic t-J-like model. Possible implications for preformed pairs formation and phase separation are drawn.Comment: 21 pages, 15 figure

    Rapid Mass Spectrometric Study of a Supercritical CO2-extract from Woody Liana Schisandra chinensis by HPLC-SPD-ESI-MS/MS

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    Woody liana Schisandra chinensis contains valuable lignans, which are phenylpropanoids with valuable biological activity. Among green and selective extraction methods, supercritical carbon dioxide (SC-CO2) was shown to be the method of choice for the recovery of these naturally occurring compounds. Carbon dioxide (CO2) was the solvent with the flow rate (10−25 g/min) with 2% ethanol as co-solvent. In this piece of work operative parameters and working conditions were optimized by experimenting with different pressures (200–400 bars) and temperatures (40–60 °C). The extraction time varied from 60 to 120 min. HPLC-SPD-ESI -MS/MS techniques were applied to detect target analytes. Twenty-six different lignans were identified in the S. chinensis SC-CO2 extracts

    Spontaneous Magnon Decays

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    A theoretical overview of the phenomenon of spontaneous magnon decays in quantum antiferromagnets is presented. The intrinsic zero-temperature damping of magnons in quantum spin systems is a fascinating many-body effect, which has recently attracted significant attention in view of its possible observation in neutron-scattering experiments. An introduction to the theory of magnon interactions and a discussion of necessary symmetry and kinematic conditions for spontaneous decays are provided. Various parallels with the decays of anharmonic phonons and excitations in superfluid 4He are extensively used. Three principal cases of spontaneous magnon decays are considered: field-induced decays in Heisenberg antiferromagnets, zero-field decays in spiral antiferromagnets, and triplon decays in quantum-disordered magnets. Analytical results are compared with available numerical data and prospective materials for experimental observation of the decay-related effects are briefly discussed.Comment: v3.0, asymptotically close to the published versio

    Thermal drag revisited: Boltzmann versus Kubo

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    The effect of mutual drag between phonons and spin excitations on the thermal conductivity of a quantum spin system is discussed. We derive general expression for the drag component of the thermal current using both Boltzmann equation approach and Kubo linear-response formalism to leading order in the spin-phonon coupling. We demonstrate that aside from higher-order corrections which appear in the Kubo formalism both approaches yield identical results for the drag thermal conductivity. We discuss the range of applicability of our result and provide a generalization of our consideration to the cases of fermionic excitations and to anomalous forms of boson-phonon coupling. Several asymptotic regimes of our findings relevant to realistic situations are highlighted.Comment: 14 pages, 3 figures, published version, extended discussio

    ИспользованиС отСчСствСнных крСмнийорганичСских ТидкостСй Π² качСствС Π½Π΅ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½Ρ‹Ρ… Ρ„Π°Π· Π² газоТидкостной Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ

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    The thermal stability of organosilicon stationary phases for gas-liquid chromatography has been tested under conditions approximating the real operation of chromatographic column.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ‹ испытания тСрмостойкости отСчСствСнных крСмнийорганичСских Π½Π΅ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½Ρ‹Ρ… Ρ„Π°Π· Π² условиях, ΠΏΡ€ΠΈΠ±Π»ΠΈΠΆΠ΅Π½Π½Ρ‹Ρ… ΠΊ ΠΎΠ±Ρ‹Ρ‡Π½Ρ‹ΠΌ условиям Ρ€Π°Π±ΠΎΡ‚Ρ‹ хроматографичСских ΠΊΠΎΠ»ΠΎΠ½Π½. Показано, Ρ‡Ρ‚ΠΎ значСния Π²Π΅Ρ€Ρ…Π½Π΅Π³ΠΎ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ³ΠΎ ΠΏΡ€Π΅Π΄Π΅Π»Π° Π±ΠΎΠ»ΡŒΡˆΠΈΠ½ΡΡ‚Π²Π° крСмнийорганичСских Π½Π΅ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½Ρ‹Ρ… Ρ„Π°Π· Π±Ρ‹Π»ΠΈ Π·Π°Π²Ρ‹ΡˆΠ΅Π½Ρ‹. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ значСния Π²Π΅Ρ€Ρ…Π½Π΅Π³ΠΎ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ³ΠΎ ΠΏΡ€Π΅Π΄Π΅Π»Π° этих Π½Π΅ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½Ρ‹Ρ… Ρ„Π°Π·, ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ соврСмСнным трСбования

    Π’Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… высококипящих элСмСнтоорганичСских соСдинСний ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ

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    Preparative gas chromatography is proposed to isolate some high-boiling organometallic compounds. Isolation of high-boiling substances should be conducted at a column temperature significantly below the boiling point, because most isolated compounds are thermally unstable at such temperatures. Stationary phases for preparative gas chromatography have a temperature limit of 350Β°C. The reduction of the column temperature is based on simultaneous changing the parameters of the chromatographic experiment (column length, impregnation degree, flow rate of the carrier gas). The influence of reducing the column temperature on the shape of the chromatographic peak is shown. The peak has an asymmetric shape, and its width increases. Therefore, the possibility of high-boiling substances preparative isolation depends on temperature decrease as the column separation efficiency is maintained.ΠœΠ΅Ρ‚ΠΎΠ΄ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ для выдСлСния Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… высококипящих элСмСнтоорганичСских соСдинСний. Π’Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ высококипящих вСщСств Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΡ‚ΡŒ ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅, Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Π½ΠΈΠΆΠ΅ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ кипСния, Ρ‚Π°ΠΊ ΠΊΠ°ΠΊ Π±ΠΎΠ»ΡŒΡˆΠΈΠ½ΡΡ‚Π²ΠΎ выдСляСмых соСдинСний тСрмичСски нСустойчивы ΠΏΡ€ΠΈ Ρ‚Π°ΠΊΠΈΡ… Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π°Ρ…. НСподвиТныС Ρ„Π°Π·Ρ‹ для ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ ΠΈΠΌΠ΅ΡŽΡ‚ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹ΠΉ ΠΏΡ€Π΅Π΄Π΅Π» 350ΒΊΠ‘. РассмотрСны особСнности выдСлСния высококипящих вСщСств ΠΏΡ€ΠΈ сниТСнии Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΈ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ кипСния вСщСства. ПониТСниС Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΈ достигнуто ΠΏΡƒΡ‚Π΅ΠΌ ΠΎΠ΄Π½ΠΎΠ²Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ измСнСния ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² хроматографичСского ΠΎΠΏΡ‹Ρ‚Π° (Π΄Π»ΠΈΠ½Ρ‹ ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΈ, стСпСни ΠΏΡ€ΠΎΠΏΠΈΡ‚ΠΊΠΈ, скорости Π³Π°Π·Π°-носитСля). Однако ΠΏΡ€ΠΈ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠΈ ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ кипСния ΠΊ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΈ Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Ρ„ΠΎΡ€ΠΌΡ‹ ΠΏΠΈΠΊΠ°, возрастаниС Π΅Π³ΠΎ ΡˆΠΈΡ€ΠΈΠ½Ρ‹. ΠŸΠΎΡΡ‚ΠΎΠΌΡƒ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ выдСлСния высококипящих вСщСств зависит ΠΎΡ‚ сниТСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΈ ΠΏΡ€ΠΈ сохранСнии эффСктивности раздСлСния

    Π’Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… органохлорсиланов ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ

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    The preparative gas chromatography method has been used for isolation and analysis of the organochlorsilanes isomers. The reaction of the organochlorsilanes with vapour of the water in the air has been studied. The method for isolation of the organochlorsilanes is proposed. It is based on using chromatographic column with efficiency up to 10000 theoretical plates. A high degree of purity (up to 99%) of the isolated compounds is achieved by an increase of separation selectivity, which is turned results from a temperature decrease. The effect of the parameters of chromatographic experiment (the column length, impregnation degree, the rate of gas-carrier) on the isolation of the compounds boiling up to 400o C was investigated.ΠœΠ΅Ρ‚ΠΎΠ΄ Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ, основанный Π½Π° использовании хроматографичСских ΠΊΠΎΠ»ΠΎΠ½ΠΎΠΊ с ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ Π΄ΠΎ 10000 тСорСтичСских Ρ‚Π°Ρ€Π΅Π»ΠΎΠΊ, ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ для выдСлСния ΠΈ Π°Π½Π°Π»ΠΈΠ·Π° Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… ΠΈΠ·ΠΎΠΌΠ΅Ρ€ΠΎΠ² органохлорсиланов, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎ Ρ€Π΅Π°Π³ΠΈΡ€ΡƒΡŽΡ‚ с Π²Π»Π°Π³ΠΎΠΉ Π²ΠΎΠ·Π΄ΡƒΡ…Π°. Высокая чистота (Π΄ΠΎ 99%) Π²Ρ‹Π΄Π΅Π»Π΅Π½Π½Ρ‹Ρ… соСдинСний достигаСтся Π·Π° счСт увСличСния сСлСктивности ΠΏΡƒΡ‚Π΅ΠΌ пониТСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹. Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ условия выдСлСния Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… ΠΈΠ·ΠΎΠΌΠ΅Ρ€ΠΎΠ² ΠΎΡ€Π³Π°Π½ΠΎ- хлорсиланов c Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π°ΠΌΠΈ кипСния Π΄ΠΎ 400ΠΎ Π‘ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ. ΠŸΠΎΠΊΠ°Π·Π°Π½Ρ‹ ΠΏΡƒΡ‚ΠΈ прСодолСния мСтодичСских трудностСй, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡŽΡ‰ΠΈΡ… ΠΏΡ€ΠΈ Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠΈ высококипящих ΠΈΠ·ΠΎΠΌΠ΅Ρ€ΠΎΠ². ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Π΄Π°Π½Π½Ρ‹Π΅ ΠΏΠΎ Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΡŽ ΠΈΠ·ΠΎΠΌΠ΅Ρ€ΠΎΠ² хлорсиланов, содСрТащих Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ Ρ€Π°Π΄ΠΈΠΊΠ°Π»Ρ‹ (ΠΌΠ΅Ρ‚ΠΈΠ»-, Π²ΠΈΠ½ΠΈΠ»-, Ρ„Π΅Π½ΠΈΠ»-, Π°Π΄Π°ΠΌΠ°Π½Ρ‚ΠΈΠ»-
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