2,370 research outputs found

    Thomas Buford Maston and the Growth of Social Christianity Among Texas Baptists

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    Locating the pseudogap closing point in cuprate superconductors: absence of entrant or reentrant behavior

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    Current descriptions of the pseudogap in underdoped cuprates envision a doping-dependent transition line T∗(p)T^*(p) which descends monotonically towards zero just beyond optimal doping. There is much debate as to the location of the terminal point p∗p^* where T∗(p)T^*(p) vanishes, whether or not there is a phase transition at T∗T^* and exactly how T∗(p)T^*(p) behaves below TcT_c within the superconducting dome. One perspective sees T∗(p)T^*(p) cutting the dome and continuing to descend monotonically to zero at pcrit≈0.19p_{crit} \approx 0.19 holes/Cu −- referred to here as `entrant behavior'. Another perspective derived from photoemission studies is that T∗(p)T^*(p) intersects the dome near pcrit≈0.23p_{crit} \approx 0.23 holes/Cu then turns back below TcT_c, falling to zero again around pcrit≈0.19p_{crit} \approx 0.19 −- referred to here as `reentrant behavior'. By examining thermodynamic data for Bi2_2Sr2_2CaCu2_2O8+δ_{8+\delta} we show that neither entrant nor reentrant behavior is experimentally supported. Rather, pcrit≈0.19p_{crit} \approx 0.19 sharply delimits the pseudogap regime and for p<0.19p < 0.19 the pseudogap is always present, independent of temperature. Similar results are found for Y0.8_{0.8}Ca0.2_{0.2}Ba2_2Cu3_3O7−δ_{7-\delta}. For both materials T∗(p)T^*(p) is not a temperature but a crossover scale, ≈E∗(p)/2kB\approx E^*(p)/2k_B, reflecting instead the underlying pseudogap energy E∗(p)E^*(p) which vanishes as p→0.19p \rightarrow 0.19.Comment: 20 Pages, 9 Figures, in press Phys. Rev.

    Review of Antarctic astronomy

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    Abstract. Astronomers have always sought the best sites for their telescopes. Antarctica, with its high plateau reaching to above 4,000 metres, intense cold, exceptionally low humidity and stable atmosphere, offers what for many forms of astronomy is the ultimate observing location on this planet. While optical, infrared and millimetre astronomers are building their observatories on the ice, particle physicists are using the ice itself as a detector and exploration of the terahertz region is being conducted from circumpolar long-duration balloons. Remarkable astronomical discoveries are already coming out of Antarctica, and much, much more is just around the corner

    UNSWIRF: A Tunable Imaging Spectrometer for the Near-Infrared

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    We describe the specifications, characteristics, calibration, and analysis of data from the University of New South Wales Infrared Fabry-Perot (UNSWIRF) etalon. UNSWIRF is a near-infrared tunable imaging spectrometer, used primarily in conjunction with IRIS on the AAT, but suitable for use as a visitor instrument at other telescopes. The etalon delivers a resolving power in excess of 4000 (corresponding to a velocity resolution ~75 km/s), and allows imaging of fields up to 100" in diameter on the AAT at any wavelength between 1.5 and 2.4 microns for which suitable blocking filters are available.Comment: 16 pages, 10 figures, uses psfig.sty and html.sty (included). To appear in Publications of the Astronomical Society of Australi

    Where is the best site on Earth? Domes A, B, C and F, and Ridges A and B

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    The Antarctic plateau contains the best sites on earth for many forms of astronomy, but none of the existing bases was selected with astronomy as the primary motivation. In this article, we try to systematically compare the merits of potential observatory sites.We include South Pole, Domes A, C, and F, and also Ridge B (running northeast from Dome A), and what we call "Ridge A" (running southwest from Dome A). Our analysis combines satellite data, published results, and atmospheric models, to compare the boundary layer, weather, aurorae, airglow, precipitable water vapor, thermal sky emission, surface temperature, and the free atmosphere, at each site. We find that all Antarctic sites are likely to be compromised for optical work by airglow and aurorae. Of the sites with existing bases, Dome A is easily the best overall; but we find that Ridge A offers an even better site. We also find that Dome F is a remarkably good site. Dome C is less good as a thermal infrared or terahertz site, but would be able to take advantage of a predicted "OH hole" over Antarctica during spring.Comment: Revised version. 16 pages, 21 figures (22 in first version). Submitted to PASP 16/05/09, accepted 13/07/09; published 20/08/0

    Significance Analysis of Time Course Microarray Experiments

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    Characterizing the genome-wide dynamic regulation of gene expression is important and will be of much interest in the future. However, there is currently no established method for identifying differentially expressed genes in a time course study. Here we propose a significance method for analyzing time course microarray studies that can be applied to the typical types of comparisons and sampling schemes. This method is applied to two studies on humans. In one study, genes are identified that show differential expression over time in response to in vivo endotoxin administration. Using our method 7409 genes are called significant at a 1% FDR level, whereas several existing approaches fail to identify any genes. In another study, 417 genes are identified at a 10% FDR level that show expression changing with age in the kidney cortex. Here it is also shown that as many as 47% of the genes change with age in a manner more complex than simple exponential growth or decay. The methodology proposed here has been implemented in the freely distributed and open-source EDGE software package

    Laminar flow of two miscible fluids in a simple network

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    When a fluid comprised of multiple phases or constituents flows through a network, non-linear phenomena such as multiple stable equilibrium states and spontaneous oscillations can occur. Such behavior has been observed or predicted in a number of networks including the flow of blood through the microcirculation, the flow of picoliter droplets through microfluidic devices, the flow of magma through lava tubes, and two-phase flow in refrigeration systems. While the existence of non-linear phenomena in a network with many inter-connections containing fluids with complex rheology may seem unsurprising, this paper demonstrates that even simple networks containing Newtonian fluids in laminar flow can demonstrate multiple equilibria. The paper describes a theoretical and experimental investigation of the laminar flow of two miscible Newtonian fluids of different density and viscosity through a simple network. The fluids stratify due to gravity and remain as nearly distinct phases with some mixing occurring only by diffusion. This fluid system has the advantage that it is easily controlled and modeled, yet contains the key ingredients for network non-linearities. Experiments and 3D simulations are first used to explore how phases distribute at a single T-junction. Once the phase separation at a single junction is known, a network model is developed which predicts multiple equilibria in the simplest of networks. The existence of multiple stable equilibria is confirmed experimentally and a criteria for their existence is developed. The network results are generic and could be applied to or found in different physical systems
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