dc magnetization measurements in fields up to 5 T on single crystals of YBa2Cu3C>7-5 reveal a well defined onset of diamagnetism allowing a unique magnetic determination of the upper critical field and its anisotropy. The upper-critical-field slopes are -1.9 and -10.5 T/K corresponding to coherence lengths of 16 and 3 A for fields perpendicular and parallel to the Cu-O planes. At the magnetically determined nucleation temperatures no distinct features are found in resistive transition curves.PACS numbers: 74.70.Vy, 74.60.EcThe values of the upper critical fields H C 2 in the high-TV superconductors are important quantities since they give the most direct information about microscopic parameters like the superconducting coherence lengths and their anisotropics within the superconducting state. So far H C 2 of YBa2Cu307-5 and other high-TV materials has been determined mainly from resistive transition curves. 1,2 However, this is complicated by an unusual broadening of the transition in a magnetic field. This behavior has been attributed to flux motion 3 ' 4 or the field dependence of the critical current in a network of Josephson junctions. 5 The flux-flow interpretation has been supported by the observation of a frequency dependence 6 of the apparent H C 2 determined by highfrequency inductive measurements and by the observation of flux creep in dc magnetization measurements. 7 These interpretations imply that resistive measurements of H C 2 yield values that are significantly lower than the equilibrium values.In order to address these issues we have carried out resistive and magnetic measurements of H c i on highquality single crystals of YBa2Cu307-5. We observe that the magnetization in a temperature interval of about 8 K ( depending on the applied field) below T c is reversible and linear in temperature, the behavior expected from 3D Ginzburg-Landau (GL) theory. Therefore these measurements reflect an equilibrium state and are not complicated by effects due to flux motion. In contrast to resistivity measurements, dc magnetization measurements in an applied field show a well defined onset of diamagnetism which allows a unique determination of the critical field. Values of H C 2 and the critical-field slopes determined in this way are considerably larger than those determined resistively. From the magnetic measurements of H C 2 we derive the superconducting parameters and the jump in the specific heat at T c which agrees well with reported experimental results. 8 Single crystals of YBa2Cu307-5 were prepared by a partial melting method. 9 Many crystals are produced in a single batch process and exhibit sharp transitions at T c > 92 K. Samples have the shape of plates with dimensions of about 0.2x2x3 mm 3 . They display patterns of twin boundaries with mm spacing which are visible with a light microscope. dc magnetization was measured with a commercial SQUID magnetometer in fields up to 5 T. In addition, magnetization measurements below 50 Oe were performed in a low-field SQUID magnetometer, ac resistivity and mag...
049ChemInform Abstract The title compound is obtained by in situ electrocrystallization of bis(ethylenedithio)tetrathiafulvalene (ET) by use of a 1:1 mixture of CuBr and tetraphenylphosphoniumdicyanamide. An X-ray analysis (space group Pnma, Z=4) shows that the structure contains alternating layers of the donor molecule cations and polymeric mixed halo(pseudohalo)cuprate(I) anions. It is established that the title compound is the organic superconductor with the highest transition temp. found to date.
Conventional disinfection and sterilization methods are often ineffective with biofilms, which are ubiquitous, hard-to-destroy microbial communities embedded in a matrix mostly composed of exopolysaccharides. The use of gas-discharge plasmas represents an alternative method, since plasmas contain a mixture of charged particles, chemically reactive species and UV radiation, whose decontamination potential for free-living, planktonic micro-organisms is well established. In this study, biofilms were produced using Chromobacterium violaceum, a Gram-negative bacterium present in soil and water and used in this study as a model organism. Biofilms were subjected to an atmospheric pressure plasma jet for different exposure times. Our results show that 99.6 % of culturable cells are inactivated after a 5 min treatment. The survivor curve shows double-slope kinetics with a rapid initial decline in c.f.u. ml "1 followed by a much slower declinewith D values that are longer than those for the inactivation of planktonic organisms, suggesting a more complex inactivation mechanism for biofilms. DNA and ATP determinations together with atomic force microscopy and fluorescence microscopy show that non-culturable cells are still alive after short plasma exposure times. These results indicate the potential of plasma for biofilm inactivation and suggest that cells go through a sequential set of physiological and morphological changes before inactivation. INTRODUCTIONMost studies dealing with the growth and physiology of bacteria have been carried out using planktonic cells in batch cultures. Although these studies have provided extensive information regarding the basic molecular mechanisms that control the growth of individual bacteria, most bacteria live primarily in communities referred to as biofilms (Stoodley et al., 2002), where cooperative effects become important. Biofilms are microbial communities embedded in a matrix mostly composed of exopolysaccharides together with some proteins and nucleic acids. Biofilm formation can be considered as a developmental cycle that begins when planktonic bacteria attach to a surface, divide and recruit additional planktonic cells that attach to the cells already on the surface. In some cases, this process results in the development of a mature biofilm, in which cells cluster in pillar-and mushroom-like structures with water channels between them, forming a primitive circulatory system (Kolter & Losick, 1998). In other cases, more compact, flat and homogeneous biofilm layers (Heydorn et al., 2000;Picioreanu et al., 2000), spherical clusters (Matsumoto et al., 2007), discrete microcolony structures (Massol-Deyá et al., 1995), ball-shaped microcolonies (Tolker-Nielsen et al., 2000) and honeycomb-like structures (Marsh et al., 2003;Russo et al., 2006) have been reported. Although it is out of the scope of this paper to extensively review the different biofilm structures reported, it is generally accepted that biofilms are not a continuous monolayer surface deposit but instead a thin base film,...
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