2,219 research outputs found
ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½ΡΡ ΠΊΠ»Π΅ΡΠΎΡΠ½ΡΡ Π°Π²ΡΠΎΠΌΠ°ΡΠΎΠ² Π΄Π»Ρ ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ Π²Π½ΡΡΡΠ΅Π½Π½Π΅ΠΉ ΡΡΡΡΠΊΡΡΡΡ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·Π° ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π° ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°
ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½ΡΡ
ΠΊΠ»Π΅ΡΠΎΡΠ½ΡΡ
Π°Π²ΡΠΎΠΌΠ°ΡΠΎΠ² ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΈΠ·ΡΡΠ΅Π½ΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·Π° ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π° ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π½Π° Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΈ ΠΏΡΠΎΡΠ½ΠΎΡΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π°, Π° ΡΠ°ΠΊΠΆΠ΅ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΡ Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ ΠΈ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠΉ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ "ΡΡΡΡΠ°Π²-ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·-Π±Π΅Π΄ΡΠ΅Π½Π½Π°Ρ ΠΊΠΎΡΡΡ". Π‘ΡΡΡΠΊΡΡΡΠ° ΠΏΡΠΎΡΠ΅Π·Π° ΠΌΠΎΠ΄ΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π»Π°ΡΡ Π²Π²Π΅Π΄Π΅Π½ΠΈΠ΅ΠΌ Π² ΡΠ΅ΠΉΠΊΡ Π΄Π΅ΠΌΠΏΡΠΈΡΡΡΡΠΈΡ
Π²ΠΊΠ»ΡΡΠ΅Π½ΠΈΠΉ ΠΈ Π½Π°Π½Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠΊΡΡΡΠΈΡ Π½Π° Π½ΠΎΠΆΠΊΡ ΠΈΠΌΠΏΠ»Π°Π½ΡΠ°ΡΠ°. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π½Π°Π»ΠΈΡΠΈΠ΅ ΡΠ°ΠΊΠΈΡ
Π²ΠΊΠ»ΡΡΠ΅Π½ΠΈΠΉ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ ΠΈΠ·ΠΌΠ΅Π½ΡΠ΅Ρ ΠΏΡΠΎΡΠ½ΠΎΡΡΡ ΡΠΈΡΡΠ΅ΠΌΡ, Π½ΠΎ ΠΏΡΠΈ ΡΡΠΎΠΌ Π²Π΅Π΄Π΅Ρ ΠΊ Π·Π°ΠΌΠ΅ΡΠ½ΠΎΠΌΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΏΡΠ΅Π΄Π΅Π»ΡΠ½ΠΎΠΉ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΡΡΡΡΠΊΡΡΡΡ "ΠΊΠΎΡΡΡ - ΠΏΡΠΎΡΠ΅Π·", Π° ΡΠ°ΠΊΠΆΠ΅ ΠΎΠΊΠ°Π·ΡΠ²Π°Π΅Ρ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΡ Π·Π°ΡΠΎΠΆΠ΄Π΅Π½ΠΈΡ ΠΈ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠΉ Π² ΠΊΠΎΡΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ
Field-cycling NMR realaxation spectroscopy of poly(di-n-alkylsiloxanes in solid, mesomorphic, and isotropic liquid phases
The frequency dependence of the proton spin-lattice relaxation times T1 and T1., in the laboratory and rotating frames, respectively, is reported for solid and liquid phases of poly(diethylsiloxane) (PDES) and in melts of poly(dimethylsiloxane) (PDMS). The total frequency range is 5 X 102 -3 X 108 Hz and is mainly covered by field-cycling NMR relaxation spectroscopy. The relaxation behavior of PDES in the liquid but ordered mesophase is compared to that of isotropic melts of PDES and PDMS and also to that of nematic main-chain liquid-crystal polymers. The frequency dependences of PDES and PDMS liquids can be represented at low and high frequencies by power laws, section by section. The relaxation behavior in the isotropic melts is entirely equivalent to that previously reported for other polymer species. In the PDES mesophase, the exponents of the power laws are significantly larger and the crossover frequency between the two regimes is reduced. The dynamics in this phase are discussed with respect to the influence of chain modes and order director fluctuations. The main conclusion is, on the whole, that data of the liquid phases are determined by chain modes rather than by local segment fluctuations. The chain dynamics in the PDES mesophase resemble the chain modes in isotropic melts modified for a microstructure with reduced randomness, whereas the influence of order director fluctuations can neither be confirmed nor ruled out
Recent NMR investigations on molecular dynamics of polymer melts in bulk and in confinement
Polymer dynamics in the melt state cover a wide range in time and frequency, for both molecular weights below and above the entanglement length. Nuclear Magnetic Resonance (NMR) offers a number of techniques that cover a broad section of this frequency range, with frequency dependent (i.e., magnetic field dependent) relaxometry providing the widest window. Combining fast field cycling techniques with frequency-temperature superposition has recently improved the understanding of polymer melt dynamics from the local to global range. At the same time, a detailed theoretical approach that separates intra- and intermolecular contributions to relaxation times has been developed. These methods are shown to improve the description of segmental dynamics in polymers, being related to time-dependent diffusion coefficients, and to distinguish between these two different relaxation contributions for a number of model compounds. The findings represent the foundation for a more thorough understanding of polymers under external restrictions and bear potential to provide a conceptually new access to biopolymer dynamics and interactions. Β© 2013 Elsevier Ltd
On the theory of double quantum NMR in polymer systems: The second cumulant approximation for many spin i = 1/2 systems
General analytical expressions for Double Quantum Nuclear Magnetic Resonance (DQ NMR) kinetic curves of many-spin I = 1/2 systems are derived with an accuracy of the second cumulant approximation. The expressions obtained exactly describe the initial part of the kinetic curves and provide a reasonable approximation up to times of about the effective spin-relaxation time. For the case when the system contains two isolated spins, this result exactly reproduces known expressions. In the case of polymer melts, the intermolecular magnetic dipole-dipole interactions significantly influence the time dependence of the DQ NMR kinetic curves. Β© 2013 AIP Publishing LLC
Anomalous diffusion and Tsallis statistics in an optical lattice
We point out a connection between anomalous quantum transport in an optical
lattice and Tsallis' generalized thermostatistics. Specifically, we show that
the momentum equation for the semiclassical Wigner function that describes
atomic motion in the optical potential, belongs to a class of transport
equations recently studied by Borland [PLA 245, 67 (1998)]. The important
property of these ordinary linear Fokker--Planck equations is that their
stationary solutions are exactly given by Tsallis distributions. Dissipative
optical lattices are therefore new systems in which Tsallis statistics can be
experimentally studied.Comment: 4 pages, 1 figur
Features of polymer chain dynamics as revealed by intermolecular nuclear magnetic dipole-dipole interaction: Model calculations and field-cycling NMR relaxometry
Proton NMR phenomena such as spin-lattice relaxation, free-induction decays, and solid echoes are analyzed with respect to contributions by intermolecular dipole-dipole interactions in polymer melts. The intermolecular dipole-dipole correlation function is calculated by taking into account the correlation hole effect characteristic for polymer melts. It is shown that the ratio between the intra- and intermolecular contributions to NMR measurands depends on the degree of isotropy of chain dynamics anticipated in different models. This, in particular, refers to the tube/reptation model that is intrinsically anisotropic in clear contrast to n -renormalized Rouse models, where no such restriction is implied. Due to anisotropy, the tube/reptation model predicts that the intramolecular contribution to the dipole-dipole correlation function increases with time relative to the intermolecular contribution. Therefore, the intramolecular contribution is expected to dominate NMR measurands by tendency at long times (or low frequencies). On the other hand, the isotropic nature of the n -renormalized Rouse model suggests that the intermolecular contribution tends to prevail on long-time scales (or low frequencies). Actually, theoretical estimations and the analysis of experimental spin-lattice relaxation data indicate that the intermolecular contribution to proton NMR measurands is no longer negligible for times longer than 10 -7s- 10-6s corresponding to frequencies below the megahertz regime. Interpretations not taking this fact into account need to be reconsidered. The systematic investigation of intermolecular interactions in long-time/low frequency proton NMR promises the revelation of the dynamic features of segment displacements relative to each other in polymer melts. Β© 2010 American Institute of Physics
ΠΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ Π²Π΅ΡΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΎΠ² Β«ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΡΒ» ΠΈ Β«innovationΒ» Π² ΡΡΡΡΠΊΠΎΠΌ ΠΈ Π°Π½Π³Π»ΠΈΠΉΡΠΊΠΎΠΌ ΡΠ·ΡΠΊΠ°Ρ (Π½Π° ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π΅ Π½Π°ΡΡΠ½ΠΎ-ΡΠ΅Ρ Π½ΠΈΡΠ΅ΡΠΊΠΈΡ ΡΠ΅ΠΊΡΡΠΎΠ²)
ΠΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ Π²Π΅ΡΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΎΠ² "ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΡ" ΠΈ "innovation" Π² ΡΡΡΡΠΊΠΎΠΌ ΠΈ Π°Π½Π³Π»ΠΈΠΉΡΠΊΠΎΠΌ ΡΠ·ΡΠΊΠ°Ρ
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Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ - ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΡΡΡΠΊΡΡΡ ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΎΠ² ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΡ ΠΈ innovation, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΡ
ΠΎΠΏΠΈΡΠ°Π½ΠΈΠ΅ ΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅.
ΠΠ±ΡΠ΅ΠΊΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β Π³ΡΡΠΏΠΏΡ ΠΏΡΠΈΠ·Π½Π°ΠΊΠΎΠ², ΠΎΠ±ΡΠ°Π·ΡΡΡΠΈΠ΅ ΡΡΡΡΠΊΡΡΡΡ ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΎΠ² ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΡ ΠΈ innovation.Concept "innovation" in Russian and English.
The aim of the work is to model the structures of concepts of innovation and innovation, as well as their description and comparison.
The object of the study is the groups of features that form the structure of concepts innovation and innovation
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