46 research outputs found
Study of the phase transition in polycrystalline (Ba_{0.90}Pb_{0.10})(Ti_{0.90}Sn_{0.10})O_3
Polycrystalline sample of (Ba_{0.90}Pb_{0.10})(Ti_{0.90}Sn_{0.10})O_3 was
obtained by means of a conventional ceramic technology. The dielectric
measurements were performed depending on temperature and frequency of electric
measuring field. The character of the phase transitions of
(Ba_{0.90}Pb_{0.10})(Ti_{0.90}Sn_{0.10})O_3 ceramics strongly depends on the
presence of Pb in the sample. The obtained results pointed out the diffused
character of phase transition. The temperature dependence of the dielectric
properties showed that the phase transition from the paraelectric phase to
ferroelectric one takes place at the same temperature (T_{m}=367 K). It does
not depend on the frequency of the measuring electric field. A change of the
value of the parameter \gamma takes place in the paraelectric phase.Comment: 5 pages, 6 figure
Elevated temperature induced dispersion phenomena in Ba1-xNaxTi1-xNbxO3
Purpose: of this paper was to investigate features of the dispersion of dielectric permittivity induced by elevated
temperature (473K-723K) in polycrystalline solid solution of Ba1-xNaxTi1-xNbxO3 (for x=0.3 and x=0.4).
Design/methodology/approach: used to perform this purpose was dielectric spectroscopy application to
measure dielectric and electric parameters within the frequency range (20Hz-1MHz).
Findings: Analysis of temperature and frequency dependences of real (ε’) and imaginary (ε”) parts of dielectric
permittivity had pointed out on relaxor type of dielectric behaviour for both investigated samples in paraelectric
phase. The thermal activation energy values of ac conductivity (for 100Hz) are similar to those of semiconductors.
Values of ε’ for both materials (x=0.3, x=0.4) are consistent with literature quotations. Thus the polarisation
behaviour of our materials seems to be similar to those described in the literature. Different behaviour of dielectric
energy losses is postulated as originating from differences of samples microstructure.
Research limitations/implications: Further investigations should be carried out in the range of low
temperatures (down to 100K) and within a broaden frequency range (up to 1.8GHz) in order to establish the
influence of chemical structure on ferroelectric-paraelectric phase transition.
Originality/value: Dielectric properties for two new material prepared from nanopowders of BaTiO3 and
NaNbO3 were described
Expression of DLK1 and MEG3 genes in porcine tissues during postnatal development
The Drosophila-like homolog 1 (DLK1), a transmembrane signal protein similar to other members of the Notch/Delta/Serrate family, regulates the differentiation process in many types of mammalian cells. Callipyge sheep and DLK1 knockout mice are excellent examples of a fundamental role of the gene encoding DLK1 in muscle growth and fat deposition. DLK1 is located within co-regulated imprinted clusters (the DLK1/DIO3 domain), along with other imprinted genes. Some of these, e.g. the RNA coding MEG3 gene, presumedly interfere with DLK1 transcription. The aim of our study was to analyze DLK1 and MEG3 gene expression in porcine tissues (muscle, liver, kidney, heart, brain stem) during postnatal development. The highest expression of both DLK1 and MEG3 variant 1 (MEG3 var.1) was observed in the brain-stem and muscles, whereas that of MEG3 variant 2 (MEG3var.2) was the most abundant in muscles and the heart. During development (between 60 and 210 days of age) expression of analyzed genes was down-regulated in all the tissues. An exception was the brain- stem, where there was no significant change in MEG3 (both variants) mRNA level, and relatively little decline (2-fold) in that of DLK1 transcription. This may indicate a distinct function of the DLK1 gene in the brain-stem, when compared with other tissues
Geographical variation in morphology of Chaetosiphella stipae stipae Hille Ris Lambers, 1947 (Hemiptera: Aphididae: Chaitophorinae)
Chaetosiphella stipae stipae is a xerothermophilous aphid, associated with Palaearctic temperate steppe zones or dry mountain valleys, where there are grasses from the genus Stipa. Its geographical distribution shows several populations that are spread from Spain, across Europe and Asia Minor, to Mongolia and China. Geographical variation in chaetotaxy and other morphological features were the basis to consider whether individuals from different populations are still the same species. Moreover, using Ch. stipae stipae and Stipa species occurrences, as well as climatic variables, we predict potential geographical distributions of the aphid and its steppe habitat. Additionally, for Stipa species we projected current climatic conditions under four climate change scenarios for 2050 and 2070. While highly variable, our results of morphometric analysis demonstrates that all Ch. stipae stipae populations are one very variable subspecies. And in view of predicted climate change, we expect reduction of Stipa grasslands. The disappearance of these ecosystems could result in stronger separation of the East-European and Asian steppes as well as European ‘warm-stage’ refuges. Therefore, the geographic morphological variability that we see today in the aphid subspecies Ch. stipae stipae may in the future lead to speciation and creation of separate subspecies or species