421 research outputs found
Competition between different order parameters in a quasi-one-dimensional superconductor
We show that, under rather general assumptions, the phase diagram of a
quasi-one-dimensional repulsive Fermi system consists of two ordered phases:
the density wave, spin or charge, and the superconductivity. It is demonstrated
that the symmetry of the superconducting order parameter is a non-universal
property sensitive to microscopic details of the model. Three potentially
stable superconducting states are identified: they are triplet -wave,
singlet -wave, and -wave. Presence of multiple competing
superconducting states implies that for a real material this symmetry is
difficult to predict theoretically and hard to probe experimentally, since
artifacts of theoretical approximations or variations in experimental
conditions could tip the balance between the superconducting phases.Comment: 6 pages, 1 eps figur
Superconductivity without attraction in a quasi-one-dimensional metal
An array of one-dimensional conductors coupled by transverse hopping and
interaction is studied with the help of a variational wave function. This wave
function is devised as to account for one-dimensional correlation effects. We
show that under broad conditions our system possesses the superconducting
ground state even if no attraction is present. The superconducting mechanism is
of many-body nature and deviates substantially from BCS. The phase diagram of
the model is mapped. It consists of two ordered phases competing against each
other: density wave, spin or charge, and unconventional superconductivity.
These phases are separated by the first order transition. The symmetry of the
superconducting order parameter is a non-universal property. It depends on
particulars of the Hamiltonian. Within the framework of our model possible
choices are the triplet -wave and the singlet -wave. Organic
quasi-one-dimensional superconductors have similar phase diagram.Comment: 12 pages, 2 Encapsulated PostScript figures, revtex4; the model's
Hamiltonian is revised as compared to previous version, this revision affects
prediction of the order parameter symmetr
ANALYSIS AND VERIFICATION OF THE OPERATION OF THE STABILIZING ROBUST CONTROLLER'S ELECTRICAL CIRCUIT OF THE ROTOR FLUX-LINKAGE CONTROL SYSTEM
On the basis of the classical theory of robust control, the theory of stability and the theory of continued fractions, the linearized mathematical model, the procedure for calculating and designing an analog electrical circuit of the Hβ-suboptimal robust controller of the flux-linkage control system of the rotor of an asynchronous electric drive, protected by Ukrainian Patent no.137157, were built. The circuit contains three operational amplifiers, several resistors and capacitors. The proposed mathematical model, the procedure for calculating and choosing the parameters of the resistors and capacitors of the circuit take into account the random variations of the object and the controller within the specified boundaries. An analytical relationship between the transfer function coefficients and the resistances of the resistors and the capacitances of the capacitors of the controller's electrical circuit was established. On a specific example, by calculation according to the developed algorithm, the limiting values of the tolerances of the circuit's resistances of the resistors and capacitances of the capacitors were identified and these values were selected with a margin from the standard series. Analysis of noise filtering by the electrical circuit of the controller in the Multisim package shows its insensitivity to noise spreads within fairly wide boundaries.Β ΠΠ° Π±Π°Π·Ρ ΠΊΠ»Π°ΡΠΈΡΠ½ΠΎΡ ΡΠ΅ΠΎΡΡΡ ΡΠΎΠ±Π°ΡΡΠ½ΠΎΠ³ΠΎ ΡΠΏΡΠ°Π²Π»ΡΠ½Π½Ρ, ΡΠ΅ΠΎΡΡΡ ΡΡΡΠΉΠΊΠΎΡΡΡ Ρ ΡΠ΅ΠΎΡΡΡ Π»Π°Π½ΡΡΠ³ΠΎΠ²ΠΈΡ
Π΄ΡΠΎΠ±ΡΠ² ΠΏΠΎΠ±ΡΠ΄ΠΎΠ²Π°Π½ΠΎ Π»ΡΠ½Π΅Π°ΡΠΈΠ·ΠΎΠ²Π°Π½Π° ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ½Π° ΠΌΠΎΠ΄Π΅Π»Ρ, ΠΏΡΠΎΡΠ΅Π΄ΡΡΠ° ΡΠΎΠ·ΡΠ°Ρ
ΡΠ½ΠΊΡ Ρ ΠΏΡΠΎΠ΅ΠΊΡΡΠ²Π°Π½Π½Ρ Π°Π½Π°Π»ΠΎΠ³ΠΎΠ²ΠΎΡ Π΅Π»Π΅ΠΊΡΡΠΈΡΠ½ΠΎΡ ΡΡ
Π΅ΠΌΠΈ Πβ-ΡΡΠ±ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΎΠ±Π°ΡΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π³ΡΠ»ΡΡΠΎΡΠ° ΡΠΈΡΡΠ΅ΠΌΠΈ ΡΠΏΡΠ°Π²Π»ΡΠ½Π½Ρ ΠΏΠΎΡΠΎΠΊΠΎΠ·ΡΠ΅ΠΏΠ»Π΅Π½Π½ΡΠΌ ΡΠΎΡΠΎΡΠ° Π°ΡΠΈΠ½Ρ
ΡΠΎΠ½Π½ΠΎΠ³ΠΎ Π΅Π»Π΅ΠΊΡΡΠΎΠΏΡΠΈΠ²ΠΎΠ΄Ρ, ΡΠΎ Π·Π°Ρ
ΠΈΡΠ΅Π½Π° ΠΏΠ°ΡΠ΅Π½ΡΠΎΠΌ Π£ΠΊΡΠ°ΡΠ½ΠΈ β 137157. Π‘Ρ
Π΅ΠΌΠ° ΠΌΡΡΡΠΈΡΡ ΡΡΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΡΠΉΠ½ΠΈΡ
ΠΏΡΠ΄ΡΠΈΠ»ΡΠ²Π°ΡΠ°, ΠΊΡΠ»ΡΠΊΠ° ΡΠ΅Π·ΠΈΡΡΠΎΡΡΠ² Ρ ΠΊΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΎΡΡΠ². ΠΠ°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½Π° ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ½Π° ΠΌΠΎΠ΄Π΅Π»Ρ, ΠΏΡΠΎΡΠ΅Π΄ΡΡΠ° ΡΠΎΠ·ΡΠ°Ρ
ΡΠ½ΠΊΡ Ρ Π²ΠΈΠ±ΠΎΡΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² ΡΠ΅Π·ΠΈΡΡΠΎΡΡΠ² Ρ ΠΊΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΎΡΡΠ² ΡΡ
Π΅ΠΌΠΈ Π²ΡΠ°Ρ
ΠΎΠ²ΡΡΡΡ Π²ΠΈΠΏΠ°Π΄ΠΊΠΎΠ²Ρ Π²Π°ΡΡΠ°ΡΡΡ ΠΎΠ±βΡΠΊΡΠ° Ρ ΡΠ΅Π³ΡΠ»ΡΡΠΎΡΠ° Π² Π·Π°Π΄Π°Π½ΠΈΡ
ΠΌΠ΅ΠΆΠ°Ρ
. ΠΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ Π°Π½Π°Π»ΡΡΠΈΡΠ½ΠΈΠΉ Π·Π²βΡΠ·ΠΎΠΊ ΠΌΡΠΆ ΠΊΠΎΠ΅ΡΡΡΡΡΠ½ΡΠ°ΠΌΠΈ ΠΏΠ΅ΡΠ΅Π΄Π°Π²Π°Π»ΡΠ½ΠΎΡ ΡΡΠ½ΠΊΡΡΡ Ρ ΠΎΠΏΠΎΡΠ°ΠΌΠΈ ΡΠ΅Π·ΠΈΡΡΠΎΡΡΠ² Ρ ΡΠΌΠ½ΠΎΡΡΡΠΌΠΈ ΠΊΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΎΡΡΠ² Π΅Π»Π΅ΠΊΡΡΠΈΡΠ½ΠΎΡ ΡΡ
Π΅ΠΌΠΈ ΡΠ΅Π³ΡΠ»ΡΡΠΎΡΠ°. ΠΠ° ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΠΎΠΌΡ ΠΏΡΠΈΠΊΠ»Π°Π΄Ρ ΡΠΎΠ·ΡΠ°Ρ
ΡΠ½ΠΊΠΎΠ²ΠΈΠΌ ΡΠ»ΡΡ
ΠΎΠΌ Π·Π° ΡΠΎΠ·ΡΠΎΠ±Π»Π΅Π½ΠΈΠΌ Π°Π»Π³ΠΎΡΠΈΡΠΌΠΎΠΌ Π²ΠΈΡΠ²Π»Π΅Π½Ρ Π³ΡΠ°Π½ΠΈΡΠ½Ρ Π·Π½Π°ΡΠ΅Π½Π½Ρ Π΄ΠΎΠΏΡΡΠΊΡΠ² ΠΎΠΏΠΎΡΡΠ² ΡΠ΅Π·ΠΈΡΡΠΎΡΡΠ² Ρ ΡΠΌΠ½ΠΎΡΡΠ΅ΠΉ ΠΊΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΎΡΡΠ² ΡΡ
Π΅ΠΌΠΈ Ρ Π·Π΄ΡΠΉΡΠ½Π΅Π½ΠΈΠΉ ΡΡ
Π²ΠΈΠ±ΡΡ ΡΠ· Π·Π°ΠΏΠ°ΡΠΎΠΌ Π·Ρ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΠΈΡ
ΡΡΠ΄ΡΠ². ΠΠ½Π°Π»ΡΠ· ΡΡΠ»ΡΡΡΠ°ΡΡΡ Π·Π°Π²Π°Π΄ Π΅Π»Π΅ΠΊΡΡΠΈΡΠ½ΠΎΡ ΡΡ
Π΅ΠΌΠΎΡ ΡΠ΅Π³ΡΠ»ΡΡΠΎΡΠ° Π² ΠΏΠ°ΠΊΠ΅ΡΡ Multisim ΠΏΠΎΠΊΠ°Π·ΡΡ ΡΡ Π½Π΅ΡΡΡΠ»ΠΈΠ²ΡΡΡΡ Π΄ΠΎ ΡΠΎΠ·ΠΌΠ°Ρ
ΡΠ² Π·Π°Π²Π°Π΄ Ρ Π΄ΠΎΡΠΈΡΡ ΡΠΈΡΠΎΠΊΠΈΡ
ΠΌΠ΅ΠΆΠ°Ρ
Quantitative comparison of planar coded aperture imaging reconstruction methods
Imaging distributions of radioactive sources plays a substantial role in nuclear medicine as well as in monitoring nuclear waste and its deposit. Coded Aperture Imaging (CAI) has been proposed as an alternative to parallel or pinhole collimators, but requires image reconstruction as an extra step. Multiple reconstruction methods with varying run time and computational complexity have been proposed. Yet, no quantitative comparison between the different reconstruction methods has been carried out so far. This paper focuses on a comparison based on three sets of hot-rod phantom images captured with an experimental Ξ³-camera consisting of a Tungsten-based MURA mask with a 2 mm thick 256 Γ 256 pixelated CdTe semiconductor detector coupled to a TimepixΒ© readout circuit. Analytical reconstruction methods, MURA Decoding, Wiener Filter and a convolutional Maximum Likelihood Expectation Maximization (MLEM) algorithm were compared to data-driven Convolutional Encoder-Decoder (CED) approaches. The comparison is based on the contrast-to-noise ratio as it has been previously used to assess reconstruction quality. For the given set-up, MURA Decoding, the most commonly used CAI reconstruction method, provides robust reconstructions despite the assumption of a linear model. For single image reconstruction, however, MLEM performed best of all analytical reconstruction methods, but took on average 45 times longer than MURA Decoding. The fastest reconstruction method is the Wiener Filter with a run time 4.3 times faster compared to MURA Decoding and a mediocre quality. The CED with a specifically tailored training set was able to succeed the most commonly used MURA decoding on average by a factor between 1.37 and 2.60 and an equal run time
Π‘ΠΈΠ½ΡΠ΅Π· Π½ΠΎΠ²ΠΈΡ ΡΠΏΡΡΠΎΡΠΈΠΊΠ»ΡΡΠ½ΠΈΡ N-Π°ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ 2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-4,6-Π΄ΡΠΎΠ½ΡΠ²
A convenient and efficient method for the synthesis of new unsaturated spiro-annulated N-aryl-4,6-dioxopyrimidine-2-thione derivatives has been developed. The resulting compounds can be potential biological active molecules or precursors for further chemical modification.Aim. To develop the methods for the synthesis of new unsaturated spiro-annulated 2-thiopyrimidine-4,6-dione derivatives, which can be used as potentially biological active molecules or precursors for their formation.Results and discussion. By condensation of N-aryl-substituted thioureas and allylmalonic acid using acetic anhydride or acetyl chloride the series of 5-allyl-substituted 2-thiopyrimidinediones has been synthesized. Their further alkylation with allyl bromide or metallyl chloride led to formation of 5,5-dialkenyl derivatives, which were converted to the corresponding unsaturated spirocyclic dioxopyrimidine-2-thiones by ring-closing metathesis.Β Experimental part. The synthesis of the starting compounds and title products was performed by preparative chemical methods, TLC and column chromatography, elemental analysis, NMR-spectroscopy.Conclusions. The efficient three-step synthetic route of new unsaturated spiro-annulated N-aryl-4,6-dioxopyrimidine-2-thione derivatives from the starting N-arylsubstituted thioureas and allylmalonic acid has been developed. The spiro-annulated products obtained can find application in biological and pharmaceutical science or as starting substrates for further chemical modification.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΡΠ΄ΠΎΠ±Π½ΡΠΉ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΡΠΈΠ½ΡΠ΅Π·Π° Π½ΠΎΠ²ΡΡ
Π½Π΅Π½Π°ΡΡΡΠ΅Π½Π½ΡΡ
ΡΠΏΠΈΡΠΎ-Π°Π½Π½Π΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
N-Π°ΡΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
2-ΡΠΈΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-4,6-Π΄ΠΈΠΎΠ½ΠΎΠ². ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΠΌΠΈ Π±ΠΈΠΎΠ°ΠΊΡΠΈΠ²Π½ΡΠΌΠΈ ΠΌΠΎΠ»Π΅ΠΊΡΠ»Π°ΠΌΠΈ ΠΈΠ»ΠΈ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠΌΠΈ Π²Π΅ΡΠ΅ΡΡΠ²Π°ΠΌΠΈ Π΄Π»Ρ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΉ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ.Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ β ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ Π½ΠΎΠ²ΡΡ
Π½Π΅Π½Π°ΡΡΡΠ΅Π½Π½ΡΡ
ΡΠΏΠΈΡΠΎ-Π°Π½Π½Π΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΡ
2-ΡΠΈΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-4,6-Π΄ΠΈΠΎΠ½Π° ΠΊΠ°ΠΊ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΡ
Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ² Π΄Π»Ρ ΠΈΡ
ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈ ΠΈΡ
ΠΎΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅. ΠΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΈΠ΅ΠΉ N-Π°ΡΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
ΡΠΈΠΎΠΌΠΎΡΠ΅Π²ΠΈΠ½ ΠΈ Π°Π»Π»ΠΈΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π³ΠΈΠ΄ΡΠΈΠ΄Π° ΠΈΠ»ΠΈ Π°ΡΠ΅ΡΠΈΠ»Ρ
Π»ΠΎΡΠΈΠ΄Π° ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ ΡΡΠ΄ 5-Π°Π»Π»ΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
2-ΡΠΈΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½Π΄ΠΈΠΎΠ½ΠΎΠ². ΠΡΠΈ ΠΈΡ
ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΌ Π°Π»ΠΊΠΈΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Π°Π»Π»ΠΈΠ»Π±ΡΠΎΠΌΠΈΠ΄ΠΎΠΌ ΠΈΠ»ΠΈ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΠ»Ρ
Π»ΠΎΡΠΈΠ΄ΠΎΠΌ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ 5,5-Π΄ΠΈΠ°Π»ΠΊΠ΅Π½ΠΈΠ»ΡΠ½ΡΠ΅ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΠ΅, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠ΅Π°ΠΊΡΠΈΡΠΌΠΈ ΠΌΠ΅ΡΠ°ΡΠ΅Π·ΠΈΡΠ° Ρ Π·Π°ΠΊΡΡΡΠΈΠ΅ΠΌ ΡΠΈΠΊΠ»Π° Π±ΡΠ»ΠΈ ΠΊΠΎΠ½Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Ρ Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠ΅ Π½Π΅ΠΏΡΠ΅Π΄Π΅Π»ΡΠ½ΡΠ΅ ΡΠΏΠΈΡΠΎΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π΄ΠΈΠΎΠΊΡΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-2-ΡΠΈΠΎΠ½Ρ.Β Β ΠΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Π°Ρ ΡΠ°ΡΡΡ. Π‘ΠΈΠ½ΡΠ΅Π· ΠΈΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΈ ΡΠ΅Π»Π΅Π²ΡΡ
ΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ² ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ Ρ
ΠΈΠΌΠΈΠΈ; ΠΎΡΠΈΡΡΠΊΠ° ΠΈ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΎΠ½ΠΊΠΎΡΠ»ΠΎΠΉΠ½ΠΎΠΉ ΠΈ ΠΊΠΎΠ»ΠΎΠ½ΠΎΡΠ½ΠΎΠΉ Ρ
ΡΠΎΠΌΠ°ΡΠΎΠ³ΡΠ°ΡΠΈΠΈ, ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°, ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠ΅ΠΉ Π―ΠΠ .ΠΡΠ²ΠΎΠ΄Ρ. Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ ΡΡΠ΅Ρ
ΡΡΠ°Π΄ΠΈΠΉΠ½ΡΠΉ ΠΏΡΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ ΠΈΠ· ΠΈΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΈΠΎΠΌΠΎΡΠ΅Π²ΠΈΠ½ ΠΈ Π°Π»Π»ΠΈΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ Π½ΠΎΠ²ΡΡ
Π½Π΅Π½Π°ΡΡΡΠ΅Π½Π½ΡΡ
ΡΠΏΠΈΡΠΎ-Π°Π½Π½Π΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΡ
N-Π°ΡΠΈΠ»-4,6-Π΄ΠΈΠΎΠΊΡΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-2-ΡΠΈΠΎΠ½Π°. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠΏΠΈΡΠΎΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΎΠ΄ΡΠΊΡΡ ΠΌΠΎΠ³ΡΡ Π½Π°ΠΉΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π² Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ ΡΠ°ΡΠΌΠ°ΡΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π½Π°ΡΠΊΠ΅, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡΡΡ ΠΊΠ°ΠΊ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠ΅ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ Π΄Π»Ρ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΉ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ.Π ΠΎΠ·ΡΠΎΠ±Π»Π΅Π½ΠΎ Π·ΡΡΡΠ½ΠΈΠΉ ΡΠ° Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΡΠΈΠ½ΡΠ΅Π·Ρ Π½ΠΎΠ²ΠΈΡ
Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½ΠΈΡ
ΡΠΏΡΡΠΎ-Π°Π½Π΅Π»ΡΠΎΠ²Π°Π½ΠΈΡ
N-Π°ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-4,6-Π΄ΡΠΎΠ½ΡΠ². ΠΠ΄Π΅ΡΠΆΠ°Π½Ρ ΡΠΏΠΎΠ»ΡΠΊΠΈ ΠΌΠΎΠΆΡΡΡ Π±ΡΡΠΈ ΠΏΠΎΡΠ΅Π½ΡΡΠΉΠ½ΠΈΠΌΠΈ Π±ΡΠΎΠ°ΠΊΡΠΈΠ²Π½ΠΈΠΌΠΈ ΠΌΠΎΠ»Π΅ΠΊΡΠ»Π°ΠΌΠΈ Π°Π±ΠΎ ΠΏΡΠ΅ΠΊΡΡΡΠΎΡΠ°ΠΌΠΈ Π΄Π»Ρ ΠΏΠΎΠ΄Π°Π»ΡΡΠΎΡ Ρ
ΡΠΌΡΡΠ½ΠΎΡ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ. ΠΠ΅ΡΠ° ΡΠΎΠ±ΠΎΡΠΈ β ΡΠΎΠ·ΡΠΎΠ±ΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΡΠ² ΠΎΠ΄Π΅ΡΠΆΠ°Π½Π½Ρ Π½ΠΎΠ²ΠΈΡ
Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½ΠΈΡ
ΡΠΏΡΡΠΎ-Π°Π½Π΅Π»ΡΠΎΠ²Π°Π½ΠΈΡ
ΠΏΠΎΡ
ΡΠ΄Π½ΠΈΡ
2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-4,6-Π΄ΡΠΎΠ½Ρ ΡΠΊ ΠΏΠΎΡΠ΅Π½ΡΡΠΉΠ½ΠΈΡ
Π±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΎ Π°ΠΊΡΠΈΠ²Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ Π°Π±ΠΎ Π½Π°ΠΏΡΠ²ΠΏΡΠΎΠ΄ΡΠΊΡΡΠ² Π΄Π»Ρ ΡΡ
ΠΎΡΡΠΈΠΌΠ°Π½Π½Ρ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΠΈ ΡΠ° ΡΡ
ΠΎΠ±Π³ΠΎΠ²ΠΎΡΠ΅Π½Π½Ρ. ΠΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΡΡΡN-Π°ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
ΡΡΠΎΡΠ΅ΡΠΎΠ²ΠΈΠ½ ΡΠ° Π°Π»ΡΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΡ ΠΊΠΈΡΠ»ΠΎΡΠΈ ΡΠ· Π·Π°ΡΡΠΎΡΡΠ²Π°Π½Π½ΡΠΌ ΠΎΡΡΠΎΠ²ΠΎΠ³ΠΎ Π°Π½Π³ΡΠ΄ΡΠΈΠ΄Ρ Π°Π±ΠΎ Π°ΡΠ΅ΡΠΈΠ»Ρ
Π»ΠΎΡΠΈΠ΄Ρ ΡΠΈΠ½ΡΠ΅Π·ΠΎΠ²Π°Π½ΠΎ ΡΠ΅ΡΡΡ 5-Π°Π»ΡΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½Π΄ΡΠΎΠ½ΡΠ². ΠΡΠΈ ΠΏΠΎΠ΄Π°Π»ΡΡΠΎΠΌΡ ΡΡ
Π°Π»ΠΊΡΠ»ΡΠ²Π°Π½Π½Ρ Π°Π»ΡΠ»Π±ΡΠΎΠΌΡΠ΄ΠΎΠΌ Π°Π±ΠΎ ΠΌΠ΅ΡΠ°Π»ΡΠ»Ρ
Π»ΠΎΡΠΈΠ΄ΠΎΠΌ ΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΎ 5,5-Π΄ΡΠ°Π»ΠΊΠ΅Π½ΡΠ»ΡΠ½Ρ ΠΏΠΎΡ
ΡΠ΄Π½Ρ, ΡΠΊΡ ΡΠ΅Π°ΠΊΡΡΡΠΌΠΈ ΠΌΠ΅ΡΠ°ΡΠ΅Π·ΠΈΡΡ ΡΠ· Π·Π°ΠΊΡΠΈΡΡΡΠΌ ΡΠΈΠΊΠ»Ρ Π±ΡΠ»ΠΎ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½ΠΎ Π½Π° Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π½Ρ Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½Ρ ΡΠΏΡΡΠΎΡΠΈΠΊΠ»ΡΡΠ½Ρ Π΄ΡΠΎΠΊΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-2-ΡΡΠΎΠ½ΠΈ.ΠΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Π° ΡΠ°ΡΡΠΈΠ½Π°. Π‘ΠΈΠ½ΡΠ΅Π· Π²ΠΈΡ
ΡΠ΄Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ ΡΠ° ΡΡΠ»ΡΠΎΠ²ΠΈΡ
ΠΏΡΠΎΠ΄ΡΠΊΡΡΠ² ΠΊΠ»Π°ΡΠΈΡΠ½ΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠ²Π½ΠΎΡ Ρ
ΡΠΌΡΡ; ΠΎΡΠΈΡΡΠΊΡ ΡΠ° ΡΠ΄Π΅Π½ΡΠΈΡΡΠΊΠ°ΡΡΡ ΠΎΡΡΠΈΠΌΠ°Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ Π·Π΄ΡΠΉΡΠ½Π΅Π½ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΎΠ½ΠΊΠΎΡΠ°ΡΠΎΠ²ΠΎΡ ΡΠ° ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΎΠ²ΠΎΡ Ρ
ΡΠΎΠΌΠ°ΡΠΎΠ³ΡΠ°ΡΡΡ, Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ½ΠΈΠΌ Π°Π½Π°Π»ΡΠ·ΠΎΠΌ, Π―ΠΠ -ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΡΡΡ.ΠΠΈΡΠ½ΠΎΠ²ΠΊΠΈ. Π ΠΎΠ·ΡΠΎΠ±Π»Π΅Π½ΠΎ Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΠΈΠΉ ΡΡΠΈΡΡΠ°Π΄ΡΠΉΠ½ΠΈΠΉ ΡΠ»ΡΡ
ΠΎΡΡΠΈΠΌΠ°Π½Π½Ρ Π· Π²ΠΈΡ
ΡΠ΄Π½ΠΈΡ
ΡΡΠΎΡΠ΅ΡΠΎΠ²ΠΈΠ½ ΡΠ° Π°Π»ΡΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΡ ΠΊΠΈΡΠ»ΠΎΡΠΈ Π½ΠΎΠ²ΠΈΡ
Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½ΠΈΡ
ΡΠΏΡΡΠΎ-Π°Π½Π΅Π»ΡΠΎΠ²Π°Π½ΠΈΡ
ΠΏΠΎΡ
ΡΠ΄Π½ΠΈΡ
N-Π°ΡΠΈΠ»-4,6-Π΄ΡΠΎΠΊΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-2-ΡΡΠΎΠ½Ρ. ΠΠ΄Π΅ΡΠΆΠ°Π½Ρ ΡΠΏΡΡΠΎΡΠΈΠΊΠ»ΡΡΠ½Ρ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈ ΠΌΠΎΠΆΡΡΡ Π·Π½Π°ΠΉΡΠΈ Π·Π°ΡΡΠΎΡΡΠ²Π°Π½Π½Ρ Π² Π±ΡΠΎΠ»ΠΎΠ³ΡΡ ΡΠ° ΡΠ°ΡΠΌΠ°ΡΠ΅Π²ΡΠΈΡΠ½ΡΠΉ Π½Π°ΡΡΡ, Π°Π±ΠΎ Π²ΠΈΠΊΠΎΡΠΈΡΡΠΎΠ²ΡΠ²Π°ΡΠΈΡΡ ΡΠΊ Π²ΠΈΡ
ΡΠ΄Π½Ρ ΡΠΏΠΎΠ»ΡΠΊΠΈ Π΄Π»Ρ ΠΏΠΎΠ΄Π°Π»ΡΡΠΎΡ Ρ
ΡΠΌΡΡΠ½ΠΎΡ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ
Kinky Behavior in Josephson Junctions
We analyze nonperturbatively the behavior of a Josephson junction in which
two BCS superconductors are coupled through an Anderson impurity. We recover
earlier perturbative results which found that a phase difference
is preferred when the impurity is singly occupied and the on-site Coulomb
interaction is large. We find a novel intermediate phase in which one of
and is stable while the other is metastable, with the
energy having a kink somewhere in between. As a consequence of the
kink, the characteristics of the junction are modified at low voltages.Comment: 7 pages, 7 encapsulated PostScript figures; figure 3 correcte
STABILITY AND ACCURACY OF THE ROBUST SYSTEM FOR STABILIZING THE ROTOR FLUX-LINKAGE OF AN ASYNCHRONOUS ELECTRIC DRIVE AT RANDOM VARIATIONS OF THE UNCERTAIN PARAMETERS WITHIN THE SPECIFIED BOUNDARIES
Purpose. The aim is to investigate the stability and the accuracy of a robust system for stabilizing the rotor flux-linkage of an asynchronous electric drive at random variations of the uncertain parameters of the object and the regulator within the specified boundaries. Methodology. To make the research, the mathematical model of the rotor flux-linkage channel of the vector control system of an asynchronous electric drive with parametric uncertainty was applied. The transfer function of the Πβ-suboptimal regulator was calculated using the mixed sensitivity method. This transfer function was used to construct the regulator structural scheme in the form of a connection of proportional and integrating links and several adders. Analytical dependences of the coefficients of the regulator's transfer function on the parameters of links of such a connection are determined. These dependences served to researching the influence of uncertain parameters of the regulator links and the object on the stability of the robust system and the accuracy of flux-linkage stabilization. Results. Investigations of the robust system stability and the accuracy of flux-linkage stabilization in the Robust Control Toolbox are done. The curves of the flux-linkage transient processes and the Bode diagram for the open system at random variations of the indeterminate parameters of the object and the regulator links within the specified boundaries are constructed. A choice of variable parameters was carried out by the Monte Carlo method. By the scatter of the obtained curves of the transient processes, the accuracy of flux-linkage stabilization was determined, and according to the Bode diagram, stability reserves in the amplitude and the phase of the robust system were determined. A high accuracy of flux-linkage stabilization (deviation less than 1 %) in fairly wide ranges of changing the uncertain parameters of the object and the regulator, while maintaining the stability of the system with permissible reserves in amplitude and phase, is established. Originality. For the first time, analytical dependences of the coefficients of the transfer function of the Πβ-suboptimal regulator on the parameters of its structural scheme, which represented in the form of a connection of proportional and integrating links, are obtained. The method for calculating the stability of a robust flux-linkage control system and the accuracy of its stabilization at random variations of the uncertain parameters of the object and the regulator links within the specified boundaries is developed. Practical value. The use of the proposed method allows, during the design of the regulator, to ensure the selection of its elements from standard series
Study Of Mass Losses Of Cauliflower At Storage Depending On A Packing Way
Tissues of fresh vegetables are characterized by the high quantity of moisture (80β¦96 %), active metabolism, low resistance to mechanical lesions, are spoiled fast. Metabolism in cells of tissues, so mass losses, depends on the content of water and dry substances.It is impossible to manage abiotic factors under conditions of open soil. So, there appears a necessity to study the influence of abiotic factors on the process of mass decrease at cauliflower storage that gives a possibility to prognosticate its mass losses and aptitude to storage.The aim of the study was to analyze the influence of weather conditions of the vegetation period of cauliflower, volume, specific mass and porosity of heads and packing methods on the intensity of natural mass losses of cauliflower at storage. The research gives a possibility to decrease natural losses of cauliflower heads and to prolong the storage duration of it. Cauliflower mass losses at the expanse of water evaporation depend on weather conditions of the vegetation period of the plant. It has been established, that there is a middle force reverse connection with the coefficient correlation r=β0,465 between the intensity of water evaporation at cauliflower heads storage and GTC, middle force connection with the coefficient correlation r=0,437 β with the average day temperature, and strong reverse connection r=β0,776 with the relative air humidity. There was elaborated the regression equation that gives an understanding about mass losses of cauliflower heads, packed in PF, at the expanse of water evaporation.The intensity of water evaporation of cauliflower at storage depends on package method. At packing in a stretch-film (SF), the intensity of moisture decrease, % a day, was the least, equal to 0,30β0,31. The ratio between moisture losses to ones of dry substances was 0,45β0,68. At packing in a performed stretch-film (PSF), the intensity of moisture decrease, % a day, was higher a little β 0,37β0,43.The more storage duration of cauliflower of late ripeness was provided by individual packing of heads in a polyethylene stretch-film. This packing type provided less total natural losses of products: in Skywoker F1β 6,0 %, in Kasper F1 and Santamaria F1 β 6,3 %. Natural losses for a day in variants with using a stretch-film were within 0,05β0,06 % depending on hybrid
Feasibility of a Small, Rapid Optical-to-IR Response, Next Generation Gamma Ray Burst Mission
We present motivations for and study feasibility of a small, rapid optical to
IR response gamma ray burst (GRB) space observatory. By analyzing existing GRB
data, we give realistic detection rates for X-ray and optical/IR instruments of
modest size under actual flight conditions. Given new capabilities of fast
optical/IR response (about 1 s to target) and simultaneous multi-band imaging,
such an observatory can have a reasonable event rate, likely leading to new
science. Requiring a Swift-like orbit, duty cycle, and observing constraints, a
Swift-BAT scaled down to 190 square cm of detector area would still detect and
locate about 27 GRB per yr. for a trigger threshold of 6.5 sigma. About 23
percent of X-ray located GRB would be detected optically for a 10 cm diameter
instrument (about 6 per yr. for the 6.5 sigma X-ray trigger).Comment: Elaborated text version of a poster presented at 2012 Malaga/Marbella
symposiu
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