110 research outputs found
Possibility of local pair existence in optimally doped SmFeAsO(1-x) in pseudogap regime
We report the analysis of pseudogap Delta* derived from resistivity
experiments in FeAs-based superconductor SmFeAsO(0.85), having a critical
temperature T_c = 55 K. Rather specific dependence Delta*(T) with two
representative temperatures followed by a minimum at about 120 K was observed.
Below T_s = 147 K, corresponding to the structural transition in SmFeAsO,
Delta*(T) decreases linearly down to the temperature T_AFM = 133 K. This last
peculiarity can likely be attributed to the antiferromagnetic (AFM) ordering of
Fe spins. It is believed that the found behavior can be explained in terms of
Machida, Nokura, and Matsubara (MNM) theory developed for the AFM
superconductors.Comment: 5 pages, 2 figure
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
Paraconductivity of K-doped SrFe2As2 superconductor
Paraconductivity of the optimally K-doped SrFe2As2 superconductor is
investigated within existing fluctuation mechanisms. The in-plane excess
conductivity has been measured in high quality single crystals, with a sharp
superconducting transition at Tc=35.5K and a transition width less than 0.3K.
The data have been also acquired in external magnetic field up to 14T. We show
that the fluctuation conductivity data in zero field and for temperatures close
to Tc, can be explained within a three-dimensional Lawrence-Doniach theory,
with a negligible Maki-Thompson contribution. In the presence of the magnetic
field, it is shown that paraconductivity obeys the three-dimensional
Ullah-Dorsey scaling law, above 2T and for H||c. The estimated upper critical
field and the coherence length nicely agree with the available experimental
data.Comment: 12 pages, 5 figure
Subthreshold antiproton production in proton-carbon reactions
Data from KEK on subthreshold antiproton as well as on pi(+-) and K(+-)
production in proton-nucleus reactions are described at projectile energies
between 3.5 and 12.0 GeV. We use a model which considers a hadron-nucleus
reaction as an incoherent sum over collisions of the projectile with a varying
number of target nucleons. It samples complete events and allows thus for the
simultaneous consideration of all particle species measured. The overall
reproduction of the data is quite satisfactory. It is shown that the
contributions from the interaction of the projectile with groups of several
target nucleons are decisive for the description of subthreshold production.
Since the collective features of subthreshold production become especially
significant far below the threshold, the results are extrapolated down to COSY
energies. It is concluded that an antiproton measurement at ANKE-COSY should be
feasible, if the high background of other particles can be efficiently
suppressed.Comment: 15 pages, 5 figures, gzipped tar file, submitted to J. Phys. G v2:
Modification of text due to demands of referee
Геномные технологии в пульмонологии: роль микроРНК в развитии бронхиальной астмы и хронической обструктивной болезни легких
MicroRNAs (miRNAs) are small noncoding RNA molecules that affect gene expression and thus take part in the epigenetic regulation of almost all physiological and pathological processes. About 1,800 human miRNAs have been discovered to date; however, biological functions and protein targets for the majority remain to be unknown. Within the respiratory system, miRNAs contribute to the lung growth and lifelong maintenance of pulmonary homeostasis. Recently, the leading role of miRNAs in pathogenesis of various pulmonary diseases has been found, including asthma, chronic obstructive pulmonary disease (COPD) and lung cancer. Due to a significant progress in studying interactions between genes and their products and environmental factors, a great role of epigenetic variability, which is gene expression change not related to DNA damage, but could be inherited consistently, became apparent. There are three levels of epigenetic regulation corresponding to three main mechanisms: genomic (DNA methylation), proteomic (histone modification) and transcriptomic (regulation through RNA, primarily miRNA). Extending our knowledge on a role of miRNAs for the respiratory system could open new therapeutic targets and diagnostic markers for respiratory diseases, particularly asthma and COPD.МикроРНК – это малые некодирующие молекулы РНК, которые влияют на экспрессию генов и таким образом участвуют в эпигенетической регуляции практически всех физиологических и патологических процессов. Примерно 1 800 микроРНК человека на сегодняшний день открыты, однако биологическая функция и белки-мишени для большинства из них остаются неизвестными. В рамках дыхательной системы микроРНК необходимы для развития легких и поддержания легочного гомеостаза на протяжении всей жизни. В последние годы была открыта главнейшая роль микроРНК в патогенезе различных заболеваний, в т. ч. бронхиальной астмы (БА), хронической обструктивной болезни легких (ХОБЛ) и рака легкого. Благодаря значительному прогрессу в изучении взаимодействий между генами и их продуктами с факторами окружающей среды стала очевидной огромная роль эпигенетической изменчивости – изменений экспрессии генов, не связанных с нарушением структуры ДНК, однако способных устойчиво передаваться в ряду поколений. Существуют 3 уровня эпигенетической регуляции и соответственно – 3 ее основных механизма: геномный (метилирование ДНК), протеомный (модификация гистонов) и транскриптомный (регуляция посредством РНК, в первую очередь микроРНК). Успехи в понимании роли микроРНК в дыхательной системе помогут пролить свет на новые перспективы в поиске терапевтических мишеней и диагностических маркеров для заболеваний респираторной системы, в частности БА и ХОБЛ
Semiconductor Spintronics
Spintronics refers commonly to phenomena in which the spin of electrons in a
solid state environment plays the determining role. In a more narrow sense
spintronics is an emerging research field of electronics: spintronics devices
are based on a spin control of electronics, or on an electrical and optical
control of spin or magnetism. This review presents selected themes of
semiconductor spintronics, introducing important concepts in spin transport,
spin injection, Silsbee-Johnson spin-charge coupling, and spindependent
tunneling, as well as spin relaxation and spin dynamics. The most fundamental
spin-dependent nteraction in nonmagnetic semiconductors is spin-orbit coupling.
Depending on the crystal symmetries of the material, as well as on the
structural properties of semiconductor based heterostructures, the spin-orbit
coupling takes on different functional forms, giving a nice playground of
effective spin-orbit Hamiltonians. The effective Hamiltonians for the most
relevant classes of materials and heterostructures are derived here from
realistic electronic band structure descriptions. Most semiconductor device
systems are still theoretical concepts, waiting for experimental
demonstrations. A review of selected proposed, and a few demonstrated devices
is presented, with detailed description of two important classes: magnetic
resonant tunnel structures and bipolar magnetic diodes and transistors. In most
cases the presentation is of tutorial style, introducing the essential
theoretical formalism at an accessible level, with case-study-like
illustrations of actual experimental results, as well as with brief reviews of
relevant recent achievements in the field.Comment: tutorial review; 342 pages, 132 figure
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