17 research outputs found
Pseudogap from ARPES experiment: three gaps in cuprates and topological superconductivity
A term first coined by Mott back in 1968 a `pseudogap' is the depletion of
the electronic density of states at the Fermi level, and pseudogaps have been
observed in many systems. However, since the discovery of the high temperature
superconductors (HTSC) in 1986, the central role attributed to the pseudogap in
these systems has meant that by many researchers now associate the term
pseudogap exclusively with the HTSC phenomenon. Recently, the problem has got a
lot of new attention with the rediscovery of two distinct energy scales
(`two-gap scenario') and charge density waves patterns in the cuprates. Despite
many excellent reviews on the pseudogap phenomenon in HTSC, published from its
very discovery up to now, the mechanism of the pseudogap and its relation to
superconductivity are still open questions. The present review represents a
contribution dealing with the pseudogap, focusing on results from angle
resolved photoemission spectroscopy (ARPES) and ends up with the conclusion
that the pseudogap in cuprates is a complex phenomenon which includes at least
three different `intertwined' orders: spin and charge density waves and
preformed pairs, which appears in different parts of the phase diagram. The
density waves in cuprates are competing to superconductivity for the electronic
states but, on the other hand, should drive the electronic structure to
vicinity of Lifshitz transition, that could be a key similarity between the
superconducting cuprates and iron based superconductors. One may also note that
since the pseudogap in cuprates has multiple origins there is no need to recoin
the term suggested by Mott.Comment: invited review, more info at http://www.imp.kiev.ua/~kor
ΠΡΡΠΈ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΠΈΠ½Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ° Π½Π° Π±Π°Π·Π΅ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ° Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ
Π ΡΠΎΠ±ΠΎΡΡ ΠΎΠΏΠΈΡΠ°Π½ΠΎ Π·Π°ΡΡΠ± Π²ΠΈΠ³ΠΎΡΠΎΠ²Π»Π΅Π½Π½Ρ ΡΠ½Π²Π΅ΡΡΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΠΌΡΠΊΡΠΎΡΠΊΠΎΠΏΡ ΡΠ»ΡΡ
ΠΎΠΌ Π΄ΠΎΡΠΎΠ±ΠΊΠΈ ΠΌΡΠΊΡΠΎΡΠΊΠΎΠΏΡ Π±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΎΠ³ΠΎ. ΠΠΏΠΈΡΠ°Π½ΠΎ ΡΠ½Π²Π΅ΡΡΠΎΠ²Π°Π½ΠΈΠΉ ΠΌΡΠΊΡΠΎΡΠΊΠΎΠΏ, ΡΡΠ²ΠΎΡΠ΅Π½ΠΈΠΉ Π½Π° Π±Π°Π·Ρ ΠΌΡΠΊΡΠΎΡΠΊΠΎΠΏΡ ΠΠΠ -3. ΠΠ°Π²Π΅Π΄Π΅Π½ΠΎ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΡ ΡΠΎΠ·ΡΠ°Ρ
ΡΠ½ΠΊΡ ΠΎΡΠ½ΠΎΠ²Π½ΠΈΡ
ΠΎΠΏΡΠΈΡΠ½ΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠ½Π²Π΅ΡΡΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΠΌΡΠΊΡΠΎΡΠΊΠΎΠΏΡ, Π²ΠΈΠΊΠΎΠ½Π°Π½ΠΎ ΡΠΎΠ·ΡΠ°Ρ
ΡΠ½ΠΊΠΈ Π΄Π»Ρ ΡΠΈΡΠΎΠΊΠΎ ΡΠΎΠ·ΠΏΠΎΠ²ΡΡΠ΄ΠΆΠ΅Π½ΠΈΡ
ΠΎΠ±βΡΠΊΡΠΈΠ²ΡΠ² Ρ ΠΎΠΊΡΠ»ΡΡΡΠ².In this work the manufacturing of the inverted microscope by the way of revision of biological microscope is described. There is described the inverted microscope manufactured on the basis of MBR-3 microscope. It contains calculations methods of the main optical specifications of the inverted microscope and the results of calculations for the most spread objectives lenses and eyepieces.Π ΡΠ°Π±ΠΎΡΠ΅ ΠΎΠΏΠΈΡΠ°Π½ ΡΠΏΠΎΡΠΎΠ± ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ ΠΈΠ½Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ° ΠΏΡΡΠ΅ΠΌ Π΄ΠΎΡΠ°Π±ΠΎΡΠΊΠΈ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ° Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ. ΠΠΏΠΈΡΠ°Π½ ΠΈΠ½Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏ, ΡΠΎΠ·Π΄Π°Π½Π½ΡΠΉ Π½Π° Π±Π°Π·Π΅ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ° ΠΠΠ -3. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΡΠ°ΡΡΠ΅ΡΠ° ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΈΠ½Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ°, Π²ΡΠΏΠΎΠ»Π½Π΅Π½Ρ ΡΠ°ΡΡΠ΅ΡΡ Π΄Π»Ρ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠΈΡΠΎΠΊΠΎ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΈΠ²ΠΎΠ² ΠΈ ΠΎΠΊΡΠ»ΡΡΠΎΠ²
Normal-superconducting transition induced by high current densities in YBa2Cu3O7-d melt-textured samples and thin films: Similarities and differences
Current-voltage characteristics of top seeded melt-textured YBa2Cu3O7-d are
presented. The samples were cut out of centimetric monoliths. Films
characteristics were also measured on microbridges patterned on thin films
grown by dc sputtering. For both types of samples, a quasi-discontinuity or
quenching was observed for a current density J* several times the critical
current density Jc. Though films and bulks much differ in their magnitude of
both Jc and J*, a proposal is made as to a common intrinsic origin of the
quenching phenomenon. The unique temperature dependence observed for the ratio
J*/Jc, as well as the explanation of the pre-quenching regime in terms of a
single dissipation model lend support to our proposal.Comment: 10 pages, 10 figures, submitted to Physical Review
Coloured nanocapsules formation process by ink-jet printing
Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ ΠΏΡΠΎΡΠ΅ΡΡ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΎΠΊΡΠ°ΡΠ΅Π½Π½ΡΡ
ΠΊΠ°ΠΏΡΡΠ» Π² ΠΏΠ»Π΅Π½ΠΊΠ°Ρ
Π°Π½ΠΎΠ΄Π½ΠΎΠ³ΠΎ
ΠΎΠΊΡΠΈΠ΄Π° Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΡΡΡΠΉΠ½ΠΎΠΉ ΠΏΠ΅ΡΠ°ΡΠΈ. ΠΠΎΠ»ΡΡΠ΅Π½Ρ ΠΎΠΊΡΠ°ΡΠ΅Π½Π½ΡΠ΅ ΡΠ»ΠΎΠΈ ΡΠΎΠ»ΡΠΈΠ½ΠΎΠΉ Π΄ΠΎ
150 ΠΌΠΊΠΌ Ρ ΡΠ°Π·ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ° 50 ΠΌΠΊΠΌ, ΠΊΠ°ΠΊ Π½Π° ΡΠΈΠΏΠΎΠ³ΡΠ°ΡΡΠΊΠΎΠΌ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠΌ Π»ΠΈΡΡΠ΅, ΡΠ°ΠΊ ΠΈ Π½Π°
ΡΠΎΠ»ΡΠ³Π΅, ΠΏΡΠΈΠ²Π°ΡΠ΅Π½Π½ΠΎΠΉ Π°Π½ΠΎΠ΄Π½ΠΎΠΉ ΡΠ²Π°ΡΠΊΠΎΠΉ ΠΊ ΡΡΠ΅ΠΊΠ»ΡΠ½Π½ΠΎΠΉ ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ΅, ΠΏΡΠΈ ΡΠ°ΡΡΠΈΡΠ½ΠΎΠΌ Π»ΠΈΠ±ΠΎ ΡΠΊΠ²ΠΎΠ·Π½ΠΎΠΌ Π°Π½ΠΎΠ΄ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΠΌ Π·Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠ΅ΠΌ Π½Π°Π½ΠΎΠΏΠΎΡ Π°Π½ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΎΠΊΡΠΈΠ΄Π°. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ ΠΎΠΊΡΠ°ΡΠ΅Π½Π½ΡΠ΅ ΡΠ»ΠΎΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡΡ ΠΈΡΠΊΠ»ΡΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠΎΠΉΠΊΠΎΡΡΡΡ. ΠΠΏΠΈΡΠ°Π½Π½ΡΠΉ Π² Π½Π°ΡΡΠΎΡΡΠ΅ΠΉ ΡΡΠ°ΡΡΠ΅ Π½ΠΈΠ·ΠΊΠΎΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΡΠΉ ΠΈ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ Π΄Π΅ΡΠ΅Π²ΡΠΉ ΠΏΡΠΎΡΠ΅ΡΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π΅Π½ Π΄Π»Ρ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠ°ΡΡΠΎΠ²ΠΎΠ³ΠΎ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π° Π΄ΠΈΡΠΏΠ»Π΅ΠΉΠ½ΡΡ
ΡΡΡΡΠΎΠΉΡΡΠ² ΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΡΠ΅Ρ
Π½ΠΈΠΊΠΈ Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΠΊΠΎΠ»Π΅Π½ΠΈΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π²ΡΡΠΎΠΊΠΎΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ "Ρ ΡΡΠ»ΠΎΠ½Π° Π½Π° ΡΡΠ»ΠΎΠ½" (roll-to-roll) ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ.The coloured capsules formation process was developed and researched by ink-jet printing in
a film of nanostructural anodic aluminum oxide. The coloured layers were obtained with thickness up
to 150 m and resolution of about 50 m at partial and through aluminum anodizing with the follow-
ing anodic oxide nanopores filling as on typographical aluminum as on foil welding to glass substrate.
Thermal and chemical stability of the obtained coloured layers were obtained. This low-temperature
inexpensive process is perspective for organization of mass display production and electronic technique elements of new generation with using of the highly productive of "roll-to-roll" technology
Tracking with capillaries and liquid scintillator
The technique of glass capillaries filled with liquid scintillator allows the reconstruction of ionizing particle tracks with high spatial resolution. Detectors based on this technique consist of coherent arrays of capillaries having diameters of the order of 20 mu m. Light signals are amplified by an optoelectronic chain composed of a series of image intensifiers: the readout is performed through a CCD. The ongoing research in the field of liquid scintillators has led to excellent results in terms of information density (greater than or equal to 5 hits/mm) and radiation resistance (order of 1 MGy). In this paper new results about the effect of ageing and purification of liquid scintillators will be presented. The RD46 collaboration has developed a completely new detector having a readout chain composed of only one image intensifier followed by a new device: a Megapixel Electron Bombarded CCD. First images of neutrino interactions will be shown, together with preliminary measurements of the resolution of the detector